Multi-axis interferometer with procedure and data processing for mirror mapping

ABSTRACT

In general, in one aspect, the invention features methods that include locating a plurality of alignment marks on a moveable stage, interferometrically measuring a position of a measurement object along an interferometer axis for each of the alignment mark locations, and using the interferometric position measurements to derive information about a surface figure of the measurement object. The position of the measurement object is measured using an interferometry assembly and either the measurement object or the interferometry assembly are attached to the stage.

CROSS-REFERENCE TO RELATED APPLICATIONS

Under 35 U.S.C. § 119(e)(1), this application claims priority to Provisional Patent Application 60/663,408, entitled “MULTI-AXIS INTERFEROMETER WITH PROCEDURE AND DATA PROCESSING FOR MIRROR MAPPING,” filed Mar. 18, 2005, the entire contents of which are hereby incorporated by reference.

TECHNICAL FIELD

This disclosure relates to interferometers, and systems and methods that use interferometers.

BACKGROUND

Displacement measuring interferometers monitor changes in the position of a measurement object relative to a reference object based on an optical interference signal. The interferometer generates the optical interference signal by overlapping and interfering a measurement beam reflected from the measurement object with a reference beam reflected from the reference object.

In many applications, the measurement and reference beams have orthogonal polarizations and different frequencies. The different frequencies can be produced, for example, by laser Zeeman splitting, by acousto-optical modulation, or internal to the laser using birefringent elements or the like. The orthogonal polarizations allow a polarizing beam-splitter to direct the measurement and reference beams to the measurement and reference objects, respectively, and combine the reflected measurement and reference beams to form overlapping exit measurement and reference beams. The overlapping exit beams form an output beam that subsequently passes through a polarizer.

The polarizer mixes polarizations of the exit measurement and reference beams to form a mixed beam. Components of the exit measurement and reference beams in the mixed beam interfere with one another so that the intensity of the mixed beam varies with the relative phase of the exit measurement and reference beams.

A detector measures the time-dependent intensity of the mixed beam and generates an electrical interference signal proportional to that intensity. Because the measurement and reference beams have different frequencies, the electrical interference signal includes a “heterodyne” signal having a beat frequency equal to the difference between the frequencies of the exit measurement and reference beams. If the lengths of the measurement and reference paths are changing relative to one another, e.g., by translating a stage that includes the measurement object, the measured beat frequency includes a Doppler shift equal to 2vnp/λ, where v is the relative speed of the measurement and reference objects, λ is the wavelength of the measurement and reference beams, n is the refractive index of the medium through which the light beams travel, e.g., air or vacuum, and p is the number of passes to the reference and measurement objects. Changes in the phase of the measured interference signal correspond to changes in the relative position of the measurement object, e.g., a change in phase of 2π corresponds substantially to a distance change d of λ/(2np). Distance 2d is a round-trip distance change or the change in distance to and from a stage that includes the measurement object. In other words, the phase Φ, ideally, is directly proportional to d, and can be expressed as $\begin{matrix} {{\Phi = {2\quad{pkd}}},{{{where}\quad k} = {\frac{2\quad\pi\quad n}{\lambda}.}}} & (1) \end{matrix}$

Unfortunately, the observable interference phase, Φ, is not always identically equal to phase Φ. Many interferometers include, for example, non-linearities such as “cyclic errors.” Cyclic errors can be expressed as contributions to the observable phase and/or the intensity of the measured interference signal and have a sinusoidal dependence on the change in for example optical path length 2pnd. In particular, a first order cyclic error in phase has for the example a sinusoidal dependence on (4πpnd)/λ and a second order cyclic error in phase has for the example a sinusoidal dependence on 2(4πpnd)/λ. Higher order cyclic errors can also be present as well as sub-harmonic cyclic errors and cyclic errors that have a sinusoidal dependence of other phase parameters of an interferometer system comprising detectors and signal processing electronics. Different techniques for quantifying such cyclic errors are described in commonly owned U.S. Pat. No. 6,137,574, U.S. Pat. No. 6,252,688, and U.S. Pat. No. 6,246,481 by Henry A. Hill.

In addition to cyclic errors, there are other sources of deviations in the observable interference phase from Φ, such as, for example, non-cyclic non-linearities or non-cyclic errors. One example of a source of a non-cyclic error is the diffraction of optical beams in the measurement paths of an interferometer. Non-cyclic error due to diffraction has been determined for example by analysis of the behavior of a system such as found in the work of J.-P. Monchalin, M. J. Kelly, J. E. Thomas, N. A. Kurnit, A. Szöke, F. Zernike, P. H. Lee, and A. Javan, “Accurate Laser Wavelength Measurement With A Precision Two-Beam Scanning Michelson Interferometer,” Applied Optics, 20(5), 736-757, 1981.

A second source of non-cyclic errors is the effect of “beam shearing” of optical beams across interferometer elements and the lateral shearing of reference and measurement beams one with respect to the other. Beam shears can be caused, for example, by a change in direction of propagation of the input beam to an interferometer or a change in orientation of the object mirror in a double pass plane mirror interferometer such as a differential plane mirror interferometer (DPMI) or a high stability plane mirror interferometer (HSPMI).

Inhomogeneities in the interferometer optics may cause wavefront errors in the reference and measurement beams. When the reference and measurement beams propagate collinearly with one another through such inhomogeneities, the resulting wavefront errors are identical and their contributions to the interferometric signal cancel each other out. More typically, however, the reference and measurement beam components of the output beam are laterally displaced from one another, i.e., they have a relative beam shear. Such beam shear causes the wavefront errors to contribute an error to the interferometric signal derived from the output beam.

Moreover, in many interferometry systems beam shear changes as the position or angular orientation of the measurement object changes. For example, a change in relative beam shear can be introduced by a change in the angular orientation of a plane mirror measurement object. Accordingly, a change in the angular orientation of the measurement object produces a corresponding error in the interferometric signal.

The effect of the beam shear and wavefront errors will depend upon procedures used to mix components of the output beam with respect to component polarization states and to detect the mixed output beam to generate an electrical interference signal. The mixed output beam may for example be detected by a detector without any focusing of the mixed beam onto the detector, by detecting the mixed output beam as a beam focused onto a detector, or by launching the mixed output beam into a single mode or multi-mode optical fiber and detecting a portion of the mixed output beam that is transmitted by the optical fiber. The effect of the beam shear and wavefront errors will also depend on properties of a beam stop should a beam stop be used in the procedure to detect the mixed output beam. Generally, the errors in the interferometric signal are compounded when an optical fiber is used to transmit the mixed output beam to the detector.

Amplitude variability of the measured interference signal can be the net result of a number of mechanisms. One mechanism is a relative beam shear of the reference and measurement components of the output beam that is for example a consequence of a change in orientation of the measurement object.

In dispersion measuring applications, optical path length measurements are made at multiple wavelengths, e.g., 532 nm and 1064 nm, and are used to measure dispersion of a gas in the measurement path of the distance measuring interferometer. The dispersion measurement can be used in converting the optical path length measured by a distance measuring interferometer into a physical length. Such a conversion can be important since changes in the measured optical path length can be caused by gas turbulence and/or by a change in the average density of the gas in the measurement arm even though the physical distance to the measurement object is unchanged.

The interferometers described above are often components of metrology systems in scanners and steppers used in lithography to produce integrated circuits on semiconductor wafers. Such lithography systems typically include a translatable stage to support and fix the wafer, focusing optics used to direct a radiation beam onto the wafer, a scanner or stepper system for translating the stage relative to the exposure beam, and one or more interferometers. Each interferometer directs a measurement beam to, and receives a reflected measurement beam from, e.g., a plane mirror attached to the stage. Each interferometer interferes its reflected measurement beams with a corresponding reference beam, and collectively the interferometers accurately measure changes in the position of the stage relative to the radiation beam. The interferometers enable the lithography system to precisely control which regions of the wafer are exposed to the radiation beam.

In many lithography systems and other applications, the measurement object includes one or more plane mirrors to reflect the measurement beam from each interferometer. Small changes in the angular orientation of the measurement object, e.g., corresponding to changes in the pitching and/or yaw of a stage, can alter the direction of each measurement beam reflected from the plane mirrors. If left uncompensated, the altered measurement beams reduce the overlap of the exit measurement and reference beams in each corresponding interferometer. Furthermore, these exit measurement and reference beams will not be propagating parallel to one another nor will their wave fronts be aligned when forming the mixed beam. As a result, the interference between the exit measurement and reference beams will vary across the transverse profile of the mixed beam, thereby corrupting the interference information encoded in the optical intensity measured by the detector.

To address this problem, many conventional interferometers include a retroreflector that redirects the measurement beam back to the plane mirror so that the measurement beam “double passes” the path between the interferometer and the measurement object. The presence of the retroreflector insures that the direction of the exit measurement is insensitive to changes in the angular orientation of the measurement object. When implemented in a plane mirror interferometer, the configuration results in what is commonly referred to as a high-stability plane mirror interferometer (HSPMI). However, even with the retroreflector, the lateral position of the exit measurement beam remains sensitive to changes in the angular orientation of the measurement object. Furthermore, the path of the measurement beam through optics within the interferometer also remains sensitive to changes in the angular orientation of the measurement object.

In practice, the interferometry systems are used to measure the position of the wafer stage along multiple measurement axes. For example, defining a Cartesian coordinate system in which the wafer stage lies in the x-y plane, measurements are typically made of the x and y positions of the stage as well as the angular orientation of the stage with respect to the z axis, as the wafer stage is translated along the x-y plane. Furthermore, it may be desirable to also monitor tilts of the wafer stage out of the x-y plane. For example, accurate characterization of such tilts may be necessary to calculate Abbé offset errors in the x and y positions. Thus, depending on the desired application, there may be up to five degrees of freedom to be measured. Moreover, in some applications, it is desirable to also monitor the position of the stage with respect to the z-axis, resulting in a sixth degree of freedom.

To measure each degree of freedom, an interferometer is used to monitor distance changes along a corresponding metrology axis. For example, in systems that measure the x and y positions of the stage as well as the angular orientation of the stage with respect to the x, y, and z axes, at least three spatially separated measurement beams reflect from one side of the wafer stage and at least two spatially separated measurement beams reflect from another side of the wafer stage. See, e.g., U.S. Pat. No. 5,801,832 entitled “METHOD OF AND DEVICE FOR REPETITIVELY IMAGING A MASK PATTERN ON A SUBSTRATE USING FIVE MEASURING AXES,” the contents of which are incorporated herein by reference. Each measurement beam is recombined with a reference beam to monitor optical path length changes along the corresponding metrology axes. Because the different measurement beams contact the wafer stage at different locations, the angular orientation of the wafer stage can then be derived from appropriate combinations of the optical path length measurements. Accordingly, for each degree of freedom to be monitored, the system includes at least one measurement beam that contacts the wafer stage. Furthermore, as described above, each measurement beam may double-pass the wafer stage to prevent changes in the angular orientation of the wafer stage from corrupting the interferometric signal. The measurement beams may be generated from physically separate interferometers or from multi-axes interferometers that generate multiple measurement beams.

SUMMARY

In addition to the sources of interferometer measurement errors discussed above, another source of measurement error in certain displacement measuring interferometry systems are variations in the surface of a plane mirror measurement object. These variations cause the mirror surface to deviate from being perfectly planar. The mirror surface shape is referred to as its surface figure, which can be characterized by a mirror surface figure function. Errors in interferometry systems that use plane mirror measurement objects can be reduced where information about the surface figure of the mirror is known. For example, knowledge of the surface figure functions allows the system to compensate for the variations in the surface figure from an ideal mirror. However, the surface figure of plane mirrors can vary with time, so the accuracy of the interferometry system measurements can degrade over the system's lifetime. Accordingly, the surface figures of the mirrors used in a metrology system should be re-measured periodically to maintain system accuracy.

Accurate knowledge of the surface figure of a plane mirror measurement object can be particularly beneficial where metrology systems are used in applications with high accuracy requirements. An example of such an application is in lithography tools where metrology systems are used to monitor the position of a stage that supports a wafer or a mask within the tool.

In some embodiments, ex situ measurement methods can be used to determine information about the surface figure of a mirror. In these methods, the mirror is removed from the lithography tool and measured using another piece of apparatus. However, the metrology system cannot be used until the mirror is replaced, so the tool is generally unproductive during such maintenance. Furthermore, the surface figure of a mirror can change when the tool is reinserted into the tool (e.g., as a result of stresses associated with the mechanical attachment of the mirror to the tool), introducing unaccounted sources of error into the metrology system.

In situ measurement methods can mitigate these errors because the surface figure is measured while it is attached to the tool, after the mirror has adapted to stresses associated with its attachment to the tool. Moreover, in situ methods can improve tool throughput by reducing the amount of time a tool is offline for servicing. In this disclosure, interferometry systems and methods are discussed in which information about a surface figure of a mirror can be obtained in a lithography tool during the operation of the tool or while the tool is offline. More generally, the systems and methods are not limited to use in lithography tools, and can be used in other applications as well (e.g., in beam writing systems).

In embodiments, procedures for determining information about a surface figure of a stage mirror includes measuring values of a second difference parameter (SDP) for the mirror. The SDP of a mirror can be expressed as a series of orthogonal basis functions (e.g., a Fourier series), where the coefficients (e.g., Fourier coefficients) of the series are related by a transfer function to corresponding coefficients of a series representation of a mirror surface figure function, ξ.

However, the SDP function is not necessarily mathematically invertible to obtain a complete set of orthogonal basis functions used in a series representation. Accordingly, additional functions are defined that, together with the SDP, allow use of a set of orthogonal basis functions which permit inversion of the SDP to a conjugate (e.g., spatial frequency) domain. These additional functions are referred to as extended SDP related parameters (SDP^(e)s).

SDP and SDP^(e)s will generally have a reduced or nominally zero sensitivity to certain spatial frequency components of a spectral representation of a surface figure where the certain spatial frequency components are related to the axis spacing of the interferometers used to measure data for the SDP and SDP^(e)s. In certain embodiments, information about the surface figure at these spatial frequency components can be acquired using supplementary methods, and the supplemental information can be used used to improve the accuracy of the surface figure determined from the SDP and SDP^(e)s.

Information about the certain spatial frequency components of the mirror surface figure can be obtained from sets of measurements in situ of an alignment wafer containing one or more nominally parallel linear arrays of alignment marks which are parallel to the surface of the stage mirror. The spacings of the alignment marks in the linear arrays are related to the spatial frequencies of components where the principle methods involving SDP and SDP^(e)s have reduced or nominally zero sensitivity.

In some embodiments, a set of measurements can be acquired corresponding to a first measurement of the positions of the alignment marks of the alignment wafer in an original position and a second measurement of positions of the alignment marks of the alignment wafer in a displaced position relative to the original position by a displacement related to a spatial frequency of components where the principle methods involving SDP and SDP^(e)s have reduced or nominally zero sensitivity.

In certain embodiments, information about the spatial frequency components where the principle methods have reduced or nominally zero sensitivity is based on sets of measurements in situ of an alignment wafer containing one or more nominally parallel linear arrays of alignment marks which are parallel to the surface of the stage mirror. For these procedures, a set of measurements corresponds to a first measurement of the positions of the alignment marks of the alignment wafer in an original orientation and a second measurement of positions of the alignment marks of the alignment wafer rotated by 180 degrees.

The values of SDP and SDP^(e)s can be measured in situ as a parallel operation with or as a serial operation with the normal processing cycle of wafers, in situ during periods other than during a normal processing cycle of wafers such as during a programmed maintenance procedure of a lithography tool, or ex-situ prior to installation of respective stage mirrors in a lithography tool. Cyclic errors that are present in the linear displacement measurements are eliminated and/or compensated by use of one of more procedures. Improved statistical accuracy in measured values of SDP and the other SDP related parameters is obtained by taking advantage of the relatively low bandwidth of measured values of SDP and the other SDP related parameters compared to the bandwidth of the corresponding linear displacement measurements using averaging or low pass filtering. Local spatial derivatives of the SDP and the other SDP related parameters are also measured using measured values of SDP and the other SDP related parameters.

There may be offset errors in SDP and the other SDP related parameters because SDP and the other SDP related parameters are derived from three different interferometer measurements where each interferometer measures only relative changes between respective reference and measurement beam paths. In addition, the offset errors may change with time because the relative path lengths of the measurement and reference beams for each of the three interferometers may change with respect to each other, e.g. due to changes in temperature. The effects of the offset errors as well as the effects of a stage rotation or rotations that may occur during the acquisition of measured values of SDP and the other SDP related parameters on subsequently determined stage mirror surface figure functions can be eliminated by use of properties of SDP relative to the other SDP related parameters. The angle or angles between the x-axis and y-axis stage mirrors appropriate to surface figure functions in one or two different x-y planes are measured by use of an alignment wafer and the alignment wafer rotated by 90 degrees. The two different planes correspond to two different planes of an interferometer system comprising two different multiple-axes/plane interferometers.

Various aspects of the invention are summarized as follows.

In general, in a first aspect, the invention features methods that include locating a plurality of alignment marks on a moveable stage, interferometrically measuring a position of a measurement object along an interferometer axis for each of the alignment mark locations, and using the interferometric position measurements to derive information about a surface figure of the measurement object. The position of the measurement object is measured using an interferometry assembly and either the measurement object or the interferometry assembly are attached to the stage.

Implementations of the methods can include one or more of the following features and/or features of other aspects. For example, The information can include information related to a certain spatial frequency component of the surface figure of the measurement object.

The method can include using the information to determine the surface figure of the measurement object. The surface figure of the measurement object can be determined based on values of a parameter associated with a displacement of the measurement object along three different measurement axes in addition to the information. The parameter values can be determined by interferometrically monitoring the displacement of the measurement object along each of the three different interferometer axes while moving the measurement object relative to the interferometry assembly, and determining the parameter values for different positions of the measurement object from the monitored displacements, wherein for a given position the parameter is based on the displacements of the measurement object along each of the three different interferometer axes at the given position.

The surface figure of the measurement object can be determined based on a frequency transform of the parameter values. The frequency transform can be a Fourier transform. The information can include information related to a certain spatial frequency component of the surface figure of the measurement object at which the frequency transform of the parameter values is substantially insensitive. The parameter can be a second difference parameter.

The plurality of alignment marks can include a linear array of alignment marks. The linear array of the alignment marks can be nominally parallel to the measurement object during the measuring. In some embodiments, adjacent alignment marks in the linear array are separated by a distance, d_(a), and the information about the surface figure of the measurement object is related to a spatial frequency component of the surface figure having a spatial wavelength Λ greater than d_(a). In certain embodiments, Λ=4d_(a).

The alignment marks can be located on the surface of an object supported by the moveable stage, and locating the alignment marks includes locating the alignment marks for at least two different positions of the object. The two different object positions can include a first position and a second position where the object is rotated 180° with respect to the first position. Alternatively, or additionally, the two different object positions can include a first position and a second position where the object is translated relative to the first position. The translation can be by an amount related to a spacing of the alignment marks.

The method can include using the information about the surface figure of the measurement object to improve the accuracy of measurements made using the interferometry assembly and the measurement object.

In some embodiments, the method includes using a lithography tool to expose a substrate supported by the moveable stage with a radiation pattern while interferometrically monitoring a distance between the interferometry assembly and the measurement object, wherein the position of the substrate relative to a reference frame is related to the distance between the interferometry assembly and the measurement object.

In another aspect, the invention features lithography methods for use in fabricating integrated circuits on a wafer. The lithography methods include supporting the wafer on a moveable stage, imaging spatially patterned radiation onto the wafer, adjusting the position of the stage, and monitoring the position of the stage using a measurement object and information about the surface figure of the measurement object derived using methods discussed in other aspects of the invention to improve the accuracy of the monitored position of the stage.

In another aspect, the invention features lithography methods for use in the fabrication of integrated circuits that include directing input radiation through a mask to produce spatially patterned radiation, positioning the mask relative to the input radiation, monitoring the position of the mask relative to the input radiation using a measurement object and information about the surface figure of the measurement object derived using methods discussed in other aspects of the invention to improve the accuracy of the monitored position of the mask, and imaging the spatially patterned radiation onto a wafer.

In a further aspect, the invention features lithography methods for fabricating integrated circuits on a wafer that include positioning a first component of a lithography system relative to a second component of a lithography system to expose the wafer to spatially patterned radiation, and monitoring the position of the first component relative to the second component using a measurement object and using information about the surface figure of the measurement object derived using methods discussed in other aspects of the invention to improve the accuracy of the monitored position of the first component.

In a further aspect, the invention features methods for fabricating integrated circuits that include applying a resist to a wafer,

forming a pattern of a mask in the resist by exposing the wafer to radiation using the lithography methods discussed in other aspects of the invention, and producing an integrated circuit from the wafer.

In general, in another aspect, the invention features systems that include a moveable stage, an alignment sensor configured to locate alignment marks associated with the moveable stage,

a interferometer assembly configured to produce three output beams each including interferometric information about a distance between the interferometer and a measurement object along a respective axis, the interferometer assembly or the measurement object being attached to the moveable stage, and an electronic processor configured to derive information about a surface figure of the measurement object based on data acquired by locating the plurality of alignment marks with the alignment sensor and measuring the position of the measurement object along one of the respective axes of the interferometer assembly for each of the alignment mark locations.

Embodiments of the system can include one or more of the following features and/or features of other aspects. For example, The measurement object can be a plane mirror. A surface of the stage can include the alignment marks. Alternatively, or additionally, the stage can be configured to support an object that includes the alignment marks.

The alignment sensor can be an optical alignment sensor, such as a microscope.

In another aspect, the invention features lithography systems for use in fabricating integrated circuits on a wafer. The lithography systems include the system disclosed above,

an illumination system for imaging spatially patterned radiation onto a wafer supported by the moveable stage, and a positioning system for adjusting the position of the stage relative to the imaged radiation. The interferometer assembly is configured to monitor the position of the wafer relative to the imaged radiation and electronic processor is configured to use the information about the surface figure of the measurement object to improve the accuracy of the monitored position of the wafer.

In a further aspect, the invention features methods for fabricating integrated circuits that include applying a resist to a wafer, forming a pattern of a mask in the resist by exposing the wafer to radiation using the lithography system discussed above, and producing an integrated circuit from the wafer.

In another aspect, the invention features beam writing systems for use in fabricating a lithography mask. The beam writing systems include the system discussed above, a source providing a write beam to pattern a substrate supported by the moveable stage, a beam directing assembly for delivering the write beam to the substrate, and a positioning system for positioning the stage and beam directing assembly relative one another. The interferometer assembly is configured to monitor the position of the stage relative to the beam directing assembly and electronic processor is configured to use the information about the surface figure of the measurement object to improve the accuracy of the monitored position of the stage.

In a further aspect, the invention features methods for fabricating a lithography mask that include directing a beam to a substrate using the beam writing system discussed above, varying the intensity or the position of the beam at the substrate to form a pattern in the substrate, and forming the lithography mask from the patterned substrate.

Other aspects and advantages of the invention will be apparent from the detailed description and the claims.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 a is a perspective drawing of an interferometer system comprising two three-axis/plane interferometers.

FIG. 1 b is a diagram that shows the pattern of measurement beams from interferometer system of FIG. 1 a at a stage mirror that serves as measurement object for interferometers of the interferometer system.

FIG. 2 a is a diagrammatic perspective view of an interferometer system.

FIG. 2 b is a diagram showing domains for a second difference parameter (SDP) and extended SDP-related parameters on a surface of a mirror.

FIG. 3 is a plot comparing the transfer function magnitude as a function of spatial frequency for different values of η.

FIG. 4 is a is a diagram that shows a linear array of alignment marks on an alignment wafer.

FIG. 5 is a schematic diagram of an embodiment of a lithography tool that includes an interferometer.

FIG. 6 a and FIG. 6 b are flow charts that describe steps for making integrated circuits.

FIG. 7 is a schematic of a beam writing system that includes an interferometry system.

Like reference symbols in the various drawings indicate like elements.

DETAILED DESCRIPTION

FIG. 1 a shows an embodiment of a multi-axis/plane mirror interferometer 100, which directs multiple measurement beams to each contact a measurement object 120 (e.g., a plane mirror measurement object) twice. Interferometer 100 produces multiple output beams 181-183 and 191-193 each including interferometric information about changes in distance between the interferometry system and the measurement object along a corresponding measurement axis.

Interferometer 100 has the property that the output beams each includes a measurement component that makes one pass to the measurement object along one of two common measurement beam paths before being directed along separate measurement beam paths for the second pass to the measurement object. Similar interferometers are disclosed in commonly owned U.S. patent application Ser. No. 10/351,707 by Henry, A. Hill filed Jan. 27, 2003 and entitled “MULTIPLE DEGREE OF FREEDOM INTERFEROMETER,” the contents of which are incorporated herein by reference.

Interferometer 100 includes a non-polarizing beam splitter 110, which splits a primary input beam 111 into two secondary input beams 112A and 112B. Interferometer 100 also includes a polarizing beam splitter 115, which splits secondary input beams 112A and 112B into primary measurement beams 113A and 113B, and primary reference beams 114A and 114B, respectively. Interferometer 100 directs primary measurement beams 113A and 113B along paths that contact measurement object 120 at different locations in a vertical direction. Similarly, primary reference beams 114A and 114B are directed along reference beam paths that contact a reference mirror 130 at different locations. Interferometer 100 also includes quarter wave plates 122 and 124. Quarter wave plate 122 is located between polarizing beam splitter 115 and measurement object 120, while quarter wave plate 124 is located between polarizing beam splitter 115 and the reference mirror. The quarter wave plates rotate by 90° the polarization state of double passed beams directed between the polarizing beam splitter and the measurement object or reference mirror. Accordingly, the polarizing beam splitter transmits an incoming beam that would have been reflected in its out-going polarization state.

The following description pertains to primary measurement beam 113A and primary reference beam 114A. Interferometer 100 directs measurement beam 113B and reference beam 114B along analogous paths. Polarizing beam splitter (PBS) 115 transmits reflected primary measurement beam 113B, which is reflected back towards PBS 115 by a retroreflector 140 (a similar retroreflector 141 reflects primary measurement beam 113B). A compound optical component 150 including non-polarizing beam splitters 151 and 152 and reflector 153 split primary measurement beam 113A into three secondary measurement beams 161, 162, and 163. PBS 115 transmits the three secondary measurement beams, which propagate along paths that contact measurement object 120 at three different positions in a horizontal plane shared by primary measurement beam 113A. PBS 115 then directs the three secondary measurement beams reflected from measurement object 120 along output paths.

PBS 115 reflects primary reference beam 114A towards retroreflector 140. As for the primary measurement beam, optical component 150 splits primary reference beam 114A reflected by retroreflector 140 into three secondary reference beams 171, 172, and 173. PBS 115 reflects secondary reference beams 171, 172, and 173 towards reference mirror 130 along paths at three different positions in a plane shared by primary reference beam 114A. PBS 115 transmits secondary reference beams 171, 172, and 173 reflected from reference object 130 along output paths so that they overlap with measurement beams 161, 162, and 163 to form output beams 181, 182, and 183, respectively. The phase of the output beams carries information about the position of the measurement object along three measurement axes defined by the primary measurement beam's path and the secondary measurement beams' paths.

Interferometer 100 also includes a window 160 located between quarter wave plate 122 and measurement object 120.

The pattern of measurement beams incident on a plane mirror measurement object is shown in FIG. 1 b. The angle of incidence of measurement beams at the mirror surface is nominally zero when the measurement axes are parallel to the x-axis of a coordinate system. The locations of the measurement axes of the top multiple-axis/plane interferometer corresponding to x₁, x₂, and x₃ are shown in FIG. 1 b. The spacings between measurement axes corresponding to x₁ and x₂ and to x₁ and x₃ are b₂ and b₃, respectively. In general, b₂ and b₃ can vary as desired. b₂ can be the same as or different from (b₃−b₂). In some embodiments, the axis spacing can be relatively narrow (e.g., about 10 cm or less, about 5 cm or less, about 3 cm or less, about 2 cm or less). For example, where the resolution of a measurement depends on the spacing the axes, having relatively narrow spacing between at least two of the measurement axes can provide increased sensitivity to higher frequencies in a measurement.

Also shown in FIG. 1 b is the location corresponding to the primary single pass measurement beam x₀′ and the locations corresponding to the second pass measurement beams x₁′, x₂′, and x₃′. The relationship between a linear displacement measurement corresponding to a double pass to the stage mirror and the linear displacement measurements corresponding to a single pass to the stage mirror is given by $\begin{matrix} {{x_{j} = {\frac{1}{2}\left( {x_{j}^{\prime} + x_{0}^{\prime}} \right)}},{j = 1},2,{{and}\quad 3.}} & (2) \end{matrix}$

The difference between two linear displacements x_(i) and x_(j), i≠j, referred to as a first difference parameter (FDP) is independent of x₀′, i.e., $\begin{matrix} {{{x_{i} - x_{j}} = {\frac{1}{2}\left( {x_{i}^{\prime} - x_{j}^{\prime}} \right)}},i,{j = 1},2,{{and}{\quad\quad}3},{i \neq {j.}}} & (3) \end{matrix}$

Reference is made to FIG. 2 a which is a diagrammatic perspective view of an interferometry system 15 that employs a pair of orthogonally arranged interferometers or interferometer subsystems by which the shape of on-stage mounted stage mirrors may be characterized in situ along one or more datum lines. As shown in FIG. 2 a, system 15 includes a stage 16 that can form part of a microlithography tool. Affixed to stage 16 is a plane stage mirror 50 having a y-z reflective surface 51 elongated in the y-direction.

Also, affixed to stage 16 is another plane stage mirror 60 having an x-z reflective surface 61 elongated in the x-direction. Mirrors 50 and 60 are mounted on stage 16 so that their reflective surfaces, 51 and 61, respectively, are nominally orthogonal to one another. Stage 16 is otherwise mounted for translations nominally in the x-y plane but may experience small angular rotations about the x, y, and z axes due to, e.g., bearing and drive mechanism tolerances. In normal operation, system 15 is adapted to be operated for scanning in the y-direction for set values of x.

Fixedly mounted off-stage (e.g., to a frame of the lithography tool) is an interferometer (or interferometer subsystem) that is generally indicated at 10. Interferometer 10 is configured to monitor the position of reflecting surface 51 along three measurement axes (e.g., x₁, x₂, and x₃) in each of two planes parallel to the x-axis, providing a measure of the position of stage 16 in the x-direction and the angular rotations of stage 16 about the y- and z-axes as stage 16 translates in the y-direction. Interferometer 10 includes two three-axis/plane interferometers such as interferometer 100 shown in FIG. 1 a and arranged so that interferometric beams travel to and from mirror 50 generally along optical paths designated generally as path 12.

Also fixedly mounted off-stage (e.g., to the frame of the lithography tool) is an interferometer (or interferometer subsystem) that is generally indicated at 20. Interferometer 20 can be used to monitor the position of reflecting surface 61 along three measurement axes (e.g., y₁, y₂, and y₃) in each of two planes parallel to the y-axis, providing a measure of the position of stage 16 in the y-direction and the angular rotations of stage 16 about the x- and z-axes as stage 16 translates in the x-direction. Interferometer 20 includes two three-axis/plane interferometers such as interferometer 100 shown in FIG. 1 a and arranged so that interferometric beams travel to and from mirror 60 generally along an optical path designated as 22.

Also shown in FIG. 2 a is an alignment sensor 14 fixedly mounted off-stage and arranged to locate alignment marks at axis 18 that are on a surface of stage 16 or on a wafer supported by stage 16. Alignment sensor 14 can be an optical sensor, such as a microscope (e.g., including a camera to monitor a field on the surface of stage 16 at axis 18). Typically, the alignment marks are protrusions or recesses in a surface that are optically distinguishable from their surroundings.

In general, simultaneously sampled values for x₁, x₂, and x₃ for x-axis stage mirror 50 are acquired as a function of position of the mirror in the y-direction with the corresponding x-axis location and the stage mirror orientation nominally held at fixed values. In addition, values for y₁, y₂, and y₃ for y-axis stage mirror 60 are measured as a function of the position in the x-direction of the y-axis stage mirror with the corresponding y-axis location and stage orientation nominally held at fixed values. The orientation of the stage can be determined initially from information obtained using one or both of the three-axis/plane interferometers.

The SDP and the SDP^(e) values for the x-axis stage mirror are calculated as a function of position of the x-axis stage mirror in the y-direction with the corresponding x-axis location and the stage mirror orientation nominally held at fixed values from the data acquired as discussed previously. Also the SDP and the SDP^(e) values for the y-axis stage mirror are measured as a function of position in the x-direction of the y-axis stage mirror with the corresponding y-axis location and stage orientation nominally held at fixed values. Increased sensitivity to high spatial frequency components of the surface figure of a stage mirror can be obtained by measuring the respective SDP and the SDP^(e) values with the stage oriented at large yaw angles and/or large measurement path lengths to the stage mirror, i.e., for large measurement beam shears at the respective measuring three-axis/plane interferometer.

The measurements of the respective SDP values for the x-axis and y-axis stage mirrors do not require monitoring of changes in stage orientation during the respective scanning of the stage mirrors other than to maintain the stage at a fixed nominal value since SDP is independent of stage mirror orientation except for third order effects. However, accurate monitoring of changes in stage orientation during scanning of a stage mirror may be required when a three-axis/plane interferometer is used to measure SDP^(e)s since these parameters may be sensitive to changes in stage orientation.

The surface figure for an x-axis stage mirror will, in general, be a function of both y and z and the surface figure for the y-axis stage mirror will, in general, be a function of both x and z. The z dependence of surface figures is suppressed in the remaining description of the data processing algorithms except where explicitly noted. The generalization to cover the z dependent properties can be addressed by using two three-axis/plane interferometer system in conjunction with a procedure to measure the angle between the x-axis and y-axis stage mirrors in two different parallel planes displaced along the z-direction corresponding to the two planes defined by the two three-axis/plane interferometer system.

The following description is given in terms of procedures used with respect to the x-axis stage mirror since the corresponding algorithms used with respect to the y-axis stage mirror can be easily obtained by a transformation of indices. Once the system has acquired values for x₁(y), x₂(y), and x₃(y) for one or more locations of the stage with respect to the x-axis, values for SDP and on or more SDP^(e)s are calculated from which ξ(y) can be determined.

Turning now to mathematical expressions for the SDP and SDP^(e), SDP can be defined for a three-axis/plane interferometer such that it is not sensitive to either a displacement of a respective mirror or to the rotation of the mirror except through a third and/or higher order effect involving the angle of stage rotation in a plane defined by the three-axis/plane interferometer and departures of the stage mirror surface from a plane.

Different combinations of displacement measurements x₁, x₂, and x₃ may be used in the definition of a SDP. One definition of a SDP for an x-axis stage mirror is for example $\begin{matrix} {{{{SDP}(y)} \equiv {\left( {x_{2} - x_{1}} \right) - {\frac{b_{2}}{b_{3} - b_{2}}\left( {x_{3} - x_{2}} \right)}}}{or}} & (4) \\ {{{{SDP}(y)} = {\left( {x_{2} - x_{1}} \right) - {\eta\left( {x_{3} - x_{2}} \right)}}}{where}} & (5) \\ {\eta \equiv {\frac{b_{2}}{b_{3} - b_{2}}.}} & (6) \end{matrix}$ Note that SDP can be written in terms of single pass displacements using Equation (3), i.e., $\begin{matrix} {{{SDP}(y)} = {{\frac{1}{2}\left\lbrack {\left( {x_{2}^{\prime} - x_{1}^{\prime}} \right) - {\eta\left( {x_{3}^{\prime} - x_{2}^{\prime}} \right)}} \right\rbrack}.}} & (7) \end{matrix}$

Of course, corresponding equations apply for a y-axis stage mirror.

The lowest order term in a series representation of the SDP is related to the second spatial derivative of a functional representation of the surface figure (e.g., corresponding to the second order term of a Taylor series representation of a surface figure). Accordingly, for relatively large spatial wavelengths, the SDP is substantially equal to the second derivative of the mirror surface figure. Generally, the SDP is determined for a line intersecting a mirror in a plane determined by the orientation of an interferometry assembly with respect to the stage mirror.

Certain properties of the three-axis/plane interferometer relevant to measurement of values of SDP are apparent. For example, SDP is independent of a displacement of the mirror for which SDP is being measured. Furthermore, SDP is generally independent of a rotation of the mirror for which SDP is being measured except through a third order or higher effects. SDP should be independent of properties of the primary single pass measurement beam path x₀′ in the three-axis/plane interferometer. SDP should be independent of properties of the retroreflector in the three-axis/plane interferometer. Furthermore, SDP should be independent of changes in the average temperature of the three-axis/plane interferometer and should be independent of linear temperature gradients in the three-axis/plane interferometer. SDP should be independent of linear spatial gradients in the refractive indices of certain components in a three-axis/plane interferometer. SDP should be independent of linear spatial gradients in the refractive indices and/or thickness of cements between components in a three-axis/plane interferometer. SDP should also be independent of “prism effects” introduced in the manufacture of components of a three-axis/plane interferometer used to measure the SDP.

SDP^(e)s are designed to exhibit spatial filtering properties of the surface figure ξ, that are similar to the spatial filtering properties of the surface figure ξ by SDP for a given portion of the respective stage mirror. SDP^(e)s can also be defined that exhibit invariance properties similar to those of SDP in procedures for determining the surface figure ξ. As a consequence of the invariance properties, neither knowledge of either the orientation of the stage mirror nor accurate knowledge of position of the stage mirror is required, e.g., accurate knowledge is not required of the position in the direction of the displacement measurements used to compute the SDP^(e)s. However, changes in the orientation of the stage mirror are monitored during the acquisition of linear displacement measurements used to determine SDP^(e)s.

SDP^(e)s can be defined such that the properties of the transfer functions with respect to the surface figure ξ is similar to the properties of the transfer function of SDP with respect to the surface figure ξ. The properties of SDP^(e)s with respect to terms of linear first pass displacement measurements is developed from knowledge of the properties of the SDP with respect to terms of linear first pass displacement measurements for a surface error function ξ that is periodic with a fundamental periodicity length L and for domains in y that are exclusive of the domain in y for which the corresponding SDP is valid. Two SDP^(e)s, denoted as SDP₁ ^(e) and SDP₂ ^(e), for a domain given by L=q2b ₃ , q=2,3, . . . ,  (8)

are given by the formulae $\begin{matrix} {{{{SDP}_{1}^{e}\left( {y,\vartheta_{z}} \right)} \equiv {{\frac{1}{2}\begin{Bmatrix} \left\lbrack {{x_{2}^{\prime}(y)} - {x_{1}^{\prime}(y)}} \right\rbrack \\ {+ {\eta\left\lbrack {{x_{2}^{\prime}(y)} - {x_{1}^{\prime}\left( {y - L + {2b_{3}}} \right)}} \right\rbrack}} \end{Bmatrix}} - {x\quad\vartheta_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{1}^{e}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}}}},{{\frac{1}{2} - \frac{2\left( {b_{3} - b_{2}} \right)}{L}} \leq \frac{y}{L} \leq \frac{1}{2}},} & (9) \\ {{{{SDP}_{2}^{e}\left( {y,\vartheta_{z}} \right)} \equiv {{{- \frac{1}{2}}\left\{ {\left\lbrack {{x_{3}^{\prime}\left( {y + L - {2b_{3}}} \right)} - {x_{2}^{\prime}(y)}} \right\rbrack + {\eta\left\lbrack {{x_{3}^{\prime}(y)} - {x_{2}^{\prime}(y)}} \right\rbrack}} \right\}} - {x\quad\vartheta_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{2}^{e}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}}}},{{- \frac{1}{2}} \leq \frac{y}{L} \leq {{- \frac{1}{2}} + {\frac{2b_{2}}{L}.}}}} & (10) \end{matrix}$ where the last term in Equations (9) and (10) is a third order term with an origin in a second order geometric term such as described in commonly owned U.S. patent application Ser. No. 10/347,271 entitled “COMPENSATION FOR GEOMETRIC EFFECTS OF BEAM MISALIGNMENTS IN PLANE MIRROR INTERFEROMETERS” and U.S. patent application Ser. No. 10/872,304 entitled “COMPENSATION FOR GEOMETRIC EFFECTS OF BEAM MISALIGNMENTS IN PLANE MIRROR INTERFEROMETER METROLOGY SYSTEMS,” both of which are by Henry A. Hill and both of which are incorporated herein in their entirety by reference.

Expressing SDP₁ ^(e) and SDP₂ ^(e) in terms of pairs of single pass displacement measurements obtained at time t_(j), j=1, 2, . . . , the following equations are derived from Equations (9) and (10): $\begin{matrix} {{{{SDP}_{1}^{e}\left( {y,\vartheta_{z}} \right)} \equiv {{\frac{1}{2}\begin{matrix} {\left( {1 + \eta} \right)\left\lbrack {{x_{2}^{\prime}\left( {y,t_{1}} \right)} - {x_{1}^{\prime}\left( {y,t_{1}} \right)}} \right\rbrack} \\ {{+ \eta}\begin{Bmatrix} \left\lbrack {{x_{3}^{\prime}\left( {{y - {2b_{3}}},t_{2}} \right)} - {x_{1}^{\prime}\left( {{y - {2b_{3}}},t_{2}} \right)}} \right\rbrack \\ {+ \left\lbrack {{x_{3}^{\prime}\left( {{y - {{2 \times 2}b_{3}}},t_{3}} \right)} - {x_{1}^{\prime}\left( {{y - {{2 \times 2}b_{3}}},t_{3}} \right)}} \right\rbrack} \\ \vdots \\ {+ \left\lbrack {{x_{3}^{\prime}\left( {{y - {\left( {q - 1} \right)2\quad b_{3}}},t_{q}} \right)} - {x_{1}^{\prime}\left( {{y - {\left( {q - 1} \right)2b_{3}}},t_{q}} \right)}} \right\rbrack} \end{Bmatrix}} \end{matrix}} - {x\quad\vartheta_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{1}^{e}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}}}},{{\frac{1}{2} - \frac{2\left( {b_{3} - b_{2}} \right)}{L}} \leq \frac{y}{L} \leq \frac{1}{2}},} & (11) \\ {{{{SDP}_{2}^{e}\left( {y,\vartheta_{z}} \right)} = {{{- \frac{1}{2}}\begin{matrix} {\left( {1 + \eta} \right)\left\lbrack {{x_{3}^{\prime}\left( {y,t_{1}} \right)} - {x_{2}^{\prime}\left( {y,t_{1}} \right)}} \right\rbrack} \\ {+ \begin{Bmatrix} {+ \left\lbrack {{x_{3}^{\prime}\left( {{y + L - {2b_{3}}},t_{2}} \right)} - {x_{1}^{\prime}\left( {{y + L - {2b_{3}}},t_{2}} \right)}} \right\rbrack} \\ \begin{matrix} {+ \left\lbrack {{x_{3}^{\prime}\left( {{y + L - {{2 \times 2}b_{3}}},t_{3}} \right)} -} \right.} \\ \left. {x_{1}^{\prime}\left( {{y + L - {{2 \times 2}b_{3}}},t_{3}} \right)} \right\rbrack \end{matrix} \\ \vdots \\ \begin{matrix} {+ \left\lbrack {{x_{3}^{\prime}\left( {{y + L - {\left( {q - 1} \right)2b_{3}}},t_{q}} \right)} -} \right.} \\ \left. {x_{1}^{\prime}\left( {{y + L - {\left( {q - 1} \right)2b_{3}}},t_{q}} \right)} \right\rbrack \end{matrix} \end{Bmatrix}} \end{matrix}} - {x\quad\vartheta_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{2}^{e}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}}}},{{- \frac{1}{2}} \leq \frac{y}{L} \leq {{- \frac{1}{2}} + \frac{2b_{2}}{L}}},} & (12) \end{matrix}$

where t_(i)≠t_(j), i≠j.

FIG. 2 b illustrate the relationship of the domains for which SDP, SDP₁ ^(e), and SDP₂ ^(e) are defined on mirror surface 51. Domain L corresponds to a portion of mirror surface 51 along a scan line 201 in the y-direction. The locations of the first pass beams on mirror surface 51 are shown for the mirror at position y_(i). Note that the domains in y for SDP, SDP₁ ^(e), and SDP₂ ^(e), i.e., ${{{- \frac{1}{2}} + \left( \frac{2b_{2}}{L} \right)} \leq \frac{y}{L} \leq {\frac{1}{2} - \left( \frac{{2b_{3}} - {2b_{2}}}{L} \right)}},{{\frac{1}{2} - \frac{\left( {{2b_{3}} - {2b_{2}}} \right)}{L}} \leq \frac{y}{L} \leq \frac{1}{2}},{{{and}{\quad\quad} - \frac{1}{2}} \leq \frac{y}{L} \leq {{- \frac{1}{2}} + \frac{2b_{2}}{L}}},$ are mutually exclusive and that the combined domains in y of the three domains cover the domain ${- \frac{1}{2}} \leq \frac{y}{L} \leq {\frac{1}{2}.}$

For a section of the x-axis stage mirror covering domain L in y, the surface figure is represented mathematically as a function ξ(y) which can be expressed by the Fourier series $\begin{matrix} {{{\xi(y)} = {{\sum\limits_{m = 0}^{N}{A_{m}{\cos\left( {m\quad 2\quad\pi\frac{y}{L}} \right)}}} + {\sum\limits_{m = 1}^{N}{B_{m}{\sin\left( {m\quad 2\quad\pi\frac{y}{L}} \right)}}}}},{{- \frac{1}{2}} \leq \frac{y}{L} \leq \frac{1}{2}},} & (13) \end{matrix}$ where N is an integer determined by consideration of the spatial frequencies that are to be included in the series representation. The term represented by A₀ which is sometimes referred to as a “piston” type error is included in Equation (13) for completeness. An error of this type is equivalent to the effect of a displacement of the stage mirror in the direction orthogonal to the stage mirror surface and as such is not considered an intrinsic property of the surface figure. Using the definition of SDP given by Equation (7), the corresponding series for SDP is next written as $\begin{matrix} {{{{SDP}\left( {x,y,\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}{{\cos\left( {m\quad 2\pi\frac{y}{L}} \right)} \times \begin{Bmatrix} {{A_{m}\left\lbrack {\left( {1 + \eta} \right) - {\cos\left( {m\quad 2\pi\quad\frac{2b_{2}}{L}} \right)} - {\eta\quad{\cos\left( {m\quad 2\quad\pi\frac{{2\quad b_{3}} - {2b_{2}}}{L}} \right)}}} \right\rbrack}\quad} \\ {+ {B_{m}\left\lbrack {{\sin\left( {m\quad 2\quad\pi\frac{2\quad b_{2}}{L}} \right)} - {\eta\quad{\sin\left( {m\quad 2\quad\pi\frac{{2\quad b_{3}} - {2b_{2}}}{L}} \right)}}} \right\rbrack}} \end{Bmatrix}}}} + {\frac{1}{2}{\sum\limits_{m = 1}^{N}{{\sin\left( {m\quad 2\pi\frac{y}{L}} \right)} \times \begin{Bmatrix} {- {A_{m}\left\lbrack {{\sin\left( {m\quad 2\quad\pi\quad\frac{2b_{2}}{L}} \right)} - {\eta\quad{\sin\left( {m\quad 2\quad\pi\frac{{2b_{3}} - {2b_{2}}}{L}} \right)}}} \right\rbrack}} \\ {+ {B_{m}\left\lbrack {\left( {1 + \eta} \right) - {\cos\left( {m\quad 2\quad\pi\frac{2\quad b_{2}}{L}} \right)} - {\eta\quad{\cos\left( {m\quad 2\pi\frac{{2b_{3}} - {2b_{2}}}{L}}\quad \right)}}} \right\rbrack}} \end{Bmatrix}}}} - {x\quad\vartheta_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}}}},{{{- \frac{1}{2}}\left( {1 - \frac{2b_{2}}{L}} \right)} \leq \frac{y}{L} \leq {\frac{1}{2}\left\lbrack {1 - \left( \frac{{2b_{3}} - {2b_{2}}}{L} \right)} \right\rbrack}},} & (14) \end{matrix}$

where x is a linear displacement of the stage mirror based on one or more of the linear displacements x_(i), i=1,2, and/or 3, and l_(z) is the angular orientation of the stage mirror in the x-y plane. The last term in Equation (14) is a third order term with an origin in a second order geometric term such as described in commonly owned U.S. patent application Ser. No. 10/347,271 entitled “COMPENSATION FOR GEOMETRIC EFFECTS OF BEAM MISALIGNMENTS IN PLANE MIRROR INTERFEROMETERS” and U.S. patent application Ser. No. 10/872,304 entitled “COMPENSATION FOR GEOMETRIC EFFECTS OF BEAM MISALIGNMENTS IN PLANE MIRROR INTERFEROMETER METROLOGY SYSTEMS,” both of which are by Henry A. Hill and both of which are incorporated herein in their entirety by reference.

The presence of the third order term in Equation (14) makes it possible to measure the high spatial frequency components of ξ(y) in the x-y plane with increased sensitivity compared to the sensitivity represented by the first order, i.e., remaining, terms in Equation (14). The third order term also makes it possible to obtain information about intermediate and low spatial frequency components of ξ, in the x-z plane complimentary to that obtained by the first order terms in Equation (14).

Note in Equation (14) that the constant term A₀ is not present. This property is subsequently used in a procedure for elimination of effects of the offset errors and changes in stage orientation. The loss of information about the constant term A₀ is not relevant to the determination of the intrinsic portion of the surface figure ξ since as noted above, A₀ corresponds to a displacement of the stage mirror in the direction orthogonal to the surface of the stage mirror.

Equation (14) may be rewritten in terms of η and b₃ and eliminating b₂ by using Equation (6) with the result $\begin{matrix} {{{{SDP}\left( {x,y,\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}{{\cos\left( {m\quad 2\pi\frac{y}{L}} \right)} \times \begin{Bmatrix} {\begin{matrix} {A_{m}\left\lbrack {\left( {1 + \eta} \right) - {\cos\left( {m\quad 2\pi\frac{\eta}{1 + \eta}\quad\frac{2b_{3}}{L}} \right)} -} \right.} \\ \left. {\eta\quad\cos\left( {m\quad 2\quad\pi\frac{1}{1 + \eta}\frac{2\quad b_{3}}{L}} \right)} \right\rbrack \end{matrix}\quad} \\ {+ {B_{m}\left\lbrack {{\sin\left( {m\quad 2\quad\pi\frac{\eta}{1 + \eta}\frac{2\quad b_{3}}{L}} \right)} - {\eta\quad{\sin\left( {m\quad 2\quad\pi\frac{1}{1 + \eta}\frac{2\quad b_{3}}{L}} \right)}}} \right\rbrack}} \end{Bmatrix}}}} + {\frac{1}{2}{\sum\limits_{m = 1}^{N}{{\sin\left( {m\quad 2\pi\frac{y}{L}} \right)} \times \begin{Bmatrix} {- {A_{m}\left\lbrack {{\sin\left( {m\quad 2\quad\pi\frac{\eta}{1 + \eta}\frac{2\quad b_{3}}{L}} \right)} - {\eta\quad{\sin\left( {m\quad 2\quad\pi\frac{1}{1 + \eta}\frac{2b_{3}}{L}} \right)}}} \right\rbrack}} \\ \begin{matrix} {+ {B_{m}\left\lbrack {\left( {1 + \eta} \right) - {\cos\left( {m\quad 2\quad\pi\frac{\eta}{1 + \eta}\frac{2\quad b_{3}}{L}} \right)}} \right.}} \\ \left. {{- \eta}\quad{\cos\left( {m\quad 2\pi\frac{1}{1 + \eta}\frac{2b_{3}}{L}}\quad \right)}} \right\rbrack \end{matrix} \end{Bmatrix}}}} - {x\quad\vartheta_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}}}},{{- {\frac{1}{2}\left\lbrack {1 - {\frac{\eta}{1 + \eta}\frac{2\quad b_{3}}{L}}} \right\rbrack}} \leq \frac{y}{L} \leq {{\frac{1}{2}\left\lbrack {1 - {\left( \frac{1}{1 + \eta} \right)\frac{2b_{3}}{L}}} \right\rbrack}.}}} & (15) \end{matrix}$

A contracted form of Equation (15) is obtained with the introduction of a complex transfer function T(m) having real and imaginary amplitudes of T_(Re) and T_(Im), respectively, as $\begin{matrix} {{{{{SDP}\left( {x,y,\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}\left\lbrack {{{\cos\left( {m\quad 2\quad\pi\quad\frac{y}{L}} \right)}A_{m}^{\prime}} + {{\sin\left( {m\quad 2\quad\pi\frac{y}{L}} \right)}B_{m}^{\prime}}} \right\rbrack}} - {x\quad\vartheta_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}}}},{{- {\frac{1}{2}\left\lbrack {1 - {\left( \frac{\eta}{1 + \eta} \right)\left( \frac{2b_{3}}{L} \right)}} \right\rbrack}} \leq \frac{y}{L} \leq {\frac{1}{2}\left\lbrack {1 - {\left( \frac{1}{1 + \eta} \right)\left( \frac{2b_{3}}{L} \right)}} \right\rbrack}}}{where}} & (16) \\ {{A_{m}^{\prime} = {{A_{m}T_{Re}} + {B_{m}T_{Im}}}}{and}} & (17) \\ {B_{m}^{\prime} = {{{- A_{m}}T_{Im}} + {B_{m}{T_{Re}.{with}}}}} & (18) \\ {{T_{Re} = \left\lbrack {\left( {1 + \eta} \right) - {\cos\left( {m\quad 2\quad\pi\frac{\eta}{1 + \eta}\frac{2b_{3}}{L}} \right)} - {\eta\quad{\cos\left( {m\quad 2\quad\pi\frac{1}{1 + \eta}\frac{2b_{3}}{L}} \right)}}} \right\rbrack},{and}} & (19) \\ {T_{Im} = {\left\lbrack {{\sin\left( {m\quad 2\quad\pi\frac{\eta}{1 + \eta}\frac{2b_{3}}{L}} \right)} - {\eta\quad{\sin\left( {m\quad 2\quad\pi\frac{1}{1 + \eta}\frac{2b_{3}}{L}} \right)}}} \right\rbrack.}} & (20) \end{matrix}$

The transfer function, T(m), relates the Fourier coefficients A′_(m) and B′_(m) of the SDP to the Fourier coefficients of ξ(y), A_(m) and B_(m). As is evident from Equations (19) and (20), T(m) depends on η and b₃/L in addition to depending on spatial frequency (as indicated by dependence on m). The dependence on spatial frequency manifests as a varying sensitivity of the transfer function to spatial frequency, with zero sensitivity occurring at certain spatial frequencies. Lack of sensitivity at a spatial frequency means that the SDP parameter does not contain any information of the mirror surface for that frequency. Subsequent calculation of the function ξ(y) should make note of these low sensitivity frequencies and handle them appropriately.

As an example, the magnitude |T(m)| of T(m) is plotted in FIG. 3 as a function of m for L=4b₃ and 2b₃=50 nm and for η= 7/4, 9/5, and 11/6. The first zero in |T(m)| for m≧1, corresponding to zero sensitivity of the transfer function, occurs at m=22, 28, and 34 for η= 7/4, 9/5, and 11/6, respectively. The spatial wavelength Λ₁=4.55, 3.57, and 2.94 mm for m=22, 28, and 34, respectively. The value of η is selected based on consideration of the corresponding spatial wavelength Λ₁, whether or not the displacements x_(i) are to be not sensitivity to spatial wavelength Λ₁ corresponding to the first zero of |T(m)|, and the diameter of the measurement beams.

There are values of η such as η= 7/4, 9/5, and 11/6 belong to one set of η's that lead to a property of measured values of x_(i) wherein the x_(i) are obtained using a corresponding three-axis/plane interferometer. The first set of η's can be expressed as a ratio of two integers that can not be reduced to a ratio of smaller integers and the numerator is an odd integer. The second set of η's are a subset of the first set of η's wherein the denominator of the ratio is an even integer. An η of the first set of η's is defined, for example, by the ratio $\begin{matrix} {{\eta = \frac{{2n} - 1}{n}},{n = 2},3,\ldots} & (21) \end{matrix}$

An η of the corresponding second set of η's is a subset of the first set of η's defined by Equation (21) for even values of η.

A property associated with this first set of η's is that the effects of the spatial frequencies corresponding the first zero of |T(m)| for m>0, i.e., corresponding to the spatial frequency that is not measured, cancel out in the linear displacements x₁ and x₂.

A property associated with the second set of η's is that the effects of the spatial frequencies corresponding the first zero of |T(m)| for m>0 cancel out in each of the linear displacements x₁, x₂, and x₃.

The first zero in |T(m)|for m≧1 and for the first set of η's is given by twice the sum of the numerator and denominator of the ratio defining an η. For the η's defined by Equation (21), the corresponding values of m for the first zero in |T(m)| for m>0 is given by the formula m=2(3n−1).  (22)

The spatial wavelength Λ₁ corresponding to the first zero in |T(m)| for m≧1 is equal to 2b₃ divided by the sum of the numerator and denominator of the ratio defining an η. For the η's defined by Equation (21), the corresponding values of Λ₁ are $\begin{matrix} {\Lambda_{1} = {\frac{2b_{3}}{{3n} - 1}.}} & (23) \end{matrix}$

The effects of the corresponding spatial frequency cancel out in x₁ and x₂ for η's of the first set of η's because the spacing b₂ between the primary first pass measurement beam and the second pass measurement beams of measurement axes x₁ and x₂ are an odd harmonic of Λ₁/2, i.e., $\begin{matrix} {b_{2} = {\left( {{2n} - 1} \right){\frac{\Lambda_{1}}{2}.}}} & (24) \end{matrix}$

The effects of the corresponding spatial frequency cancel out in x₁, x₂, and x₃ for η's of the second set of η's because the spacing b₂ between the primary first pass measurement beam and the second pass measurement beams of measurement axes x₁ and x₂ and the spacing (2b₃−b₂) between the primary first pass measurement beam and the second pass measurement beam of measurement axis x₃ are each an odd harmonic of Λ₁/2, i.e., spacing b₂ is given by Equation (24) and spacing (2b₃−b₂) is given by the equation $\begin{matrix} {\left( {{2b_{3}} - b_{2}} \right) = {\left( {{4n} - 1} \right){\frac{\Lambda_{1}}{2}.}}} & (25) \end{matrix}$

There are other values of η's that belong to the first set which are given by the formulae $\begin{matrix} {{\eta = \frac{{2n} + 1}{n}},{n\quad = 2},3,\ldots} & (26) \end{matrix}$

The corresponding values for Λ₁, b₂, and (2b₃−b₂) are $\begin{matrix} {\Lambda_{1} = \frac{2b_{3}}{{3n} + 1}} & (27) \\ {{b_{2} = {\left( {{2n} + 1} \right)\frac{\Lambda_{1}}{2}}},} & (28) \\ {\left( {{2b_{3}} - b_{2}} \right) = {\left( {{4n} + 1} \right){\frac{\Lambda_{1}}{2}.}}} & (29) \end{matrix}$

Other values of η's that belong to the second set are given by the formulae $\begin{matrix} {{\eta = \frac{{2n} \pm 1}{2n}},{n = 2},3,\ldots} & (30) \end{matrix}$

The corresponding values for Λ₁, b₂, and (2b₃−b₂) are $\begin{matrix} {{\Lambda_{1} = \frac{2b_{3}}{{4n} \pm 1}},} & (31) \\ {{b_{2} = {\left( {{2n} \pm 1} \right)\frac{\Lambda_{1}}{2}}},} & (32) \\ {\left( {{2b_{3}} - b_{2}} \right) = {\left( {{6n} \pm 1} \right){\frac{\Lambda_{1}}{2}.}}} & (33) \end{matrix}$

It was noted in the discussion associated with Equations (14), (15), (16), and (17) that the effects of the spatial frequency component with a spatial wavelength of Λ₁ cancel out in x₁, x₂, and x₃ for η's of the second set of η's. This is because the spacing b₂ between the primary first pass measurement beam and the second pass measurement beams of measurement axes x₁ and x₂ and the spacing (2b₃−b₂) between the primary first pass measurement beam and the second pass measurement beam of measurement axis x₃ are each an odd harmonic of Λ₁/2. However, this advantage may not be realized in certain end use applications as a result of errors introduced in manufacturing the interferometer. The manufacturing errors alter for example the locations of the measurement beams which in turn introduce errors in η such that the condition of Equation (13) may not be satisfied. When the effects of the spatial frequency components with a spatial wavelength of Λ₁ and other similar spatial wavelengths do not cancel out in x₁, x₂, and x₃, the amplitudes of the spatial frequency components are measured in subsequently described procedures based on measurements of an alignment wafer. These procedures will hereinafter be referred to as alignment wafer procedures.

The cut off spatial frequency in the determination of the surface figure properties represented by ξ when using the three-axis/plane interferometer will be determined by the spatial filtering properties of measurement beams having a finite diameter, i.e., the finite size of a measurement beam will serve as a low pass filter with respect to effects of the higher frequency spatial frequencies of ξ. These effects are evaluated here for a measurement beam with a Gaussian profile. For a Gaussian profile with a 1/e² diameter of 2s with respect to beam intensity, the effect of the spatial filtering of a Fourier series component with a spatial wavelength Λ is given by a transfer function T_(Beam) where $\begin{matrix} {T_{Beam} = {{\mathbb{e}}^{{- {(\frac{\pi^{2}}{8})}}{(\frac{2s}{\Lambda})}^{2}}.}} & (34) \end{matrix}$

Consider for example the effect of a Gaussian beam profile with a 1/e² diameter of 2s=5.0 mm. The attenuation effect of the spatial filtering will be 0.225, 0.089, and 0.028 for Λ=4.55, 3.57, and 2.94 mm, respectively, for the respective Fourier series component amplitudes.

Using Equations (9) and (10), the series representations of SDP₁ ^(e) and SDP₂ ^(e) for the Fourier series representation of ξ(y) given by Equation (13) are $\begin{matrix} {{{{SDP}_{1}^{e}\left( {x,y,\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}\left\lbrack {{{\cos\left( {{m2}\quad\pi\frac{y}{L}} \right)}A_{m}^{\prime}} + {{\sin\left( {m\quad 2\pi\frac{y}{L}} \right)}B_{m}^{\prime}}} \right\rbrack}} + {\eta\frac{L}{2}\vartheta_{z}} - {x\quad\vartheta_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{1}^{e}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}}}},{{\frac{1}{2}\left\lbrack {1 - {2\left( \frac{1}{1 + \eta} \right)\left( \frac{2b_{3}}{L} \right)}} \right\rbrack} \leq \frac{y}{L} \leq \frac{1}{2}},} & (35) \\ {{{{SDP}_{2}^{e}\left( {x,y,\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}\left\lbrack {{{\cos\left( {m\quad 2\quad\pi\frac{y}{L}} \right)}A_{m}^{\prime}} + {{\sin\left( {m\quad 2\pi\frac{y}{L}} \right)}B_{m}^{\prime}}} \right\rbrack}} - {\frac{L}{2}\quad\vartheta_{z}} - {x\quad\vartheta_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{2}^{e}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}}}},{{- \frac{1}{2}} \leq \frac{y}{L} \leq {- {{\frac{1}{2}\left\lbrack {1 - {2\left( \frac{\eta}{1 + \eta} \right)\left( \frac{2b_{3}}{L} \right)}} \right\rbrack}.}}}} & (36) \end{matrix}$

Note in Equations (35) and (36) that the constant term A₀ is not present. The discussion of this feature relevant to the intrinsic surface figure function is the same as the corresponding portion of the discussion related to the constant term A₀ not being included in Equation (14).

From a comparison of Equations (35) and (36), another property of SDP₁ ^(e) and SDP₂ ^(e) is evident, i.e., the respective contributions of the Fourier series terms in A_(m)′ and B_(m)′are the same in SDP₁ ^(e) and SDP₂ ^(e). Furthermore, the respective contributions of the Fourier series terms in A_(m)′ and B_(m)′ in SDP₁ ^(e) and SDP₂ ^(e) are the same as the respective contributions in SDP (see Equation (16)).

The SDP₁ ^(e) and SDP₂ ^(e) are classified as conjugate other SDP related parameters because of the cited property and because the first order terms ηLl_(z) and −Ll_(Z), respectively, multiplied by the respective domains in y, i.e., 2 b₃/(1+η) and 2ηb₃/(1+η), respectively, are equal in magnitude and have opposite signs.

While certain SDP^(e)s have been explicitly defined, there are also other SDP^(e)s for L=4b₃+q2b₂+p2(b₃−b₂), q=1,2, . . . , p=1,2, . . . , that exhibit similar properties as those of identified with respect to SDP₁ ^(e) and SDP₂ ^(e), such as an invariance to displacements of the stage mirror as evident on inspection of Equations (11) and (12). Another property of SDP₁ ^(e) and SDP₂ ^(e) is that the effect of a stage rotation and the corresponding changes in SDP₁ ^(e) and SDP₂ ^(e) multiplied by their respective domain widths in y are equal in magnitude but opposite in signs. This property is evident on examination of Equations (35) and (36).

In some embodiments, the effects of the offset errors and the effects of changes in l_(z) that occur during the measurements of x₁(y), x₂(y), and x₃(y) are next included in the representations of SDP, SDP₁ ^(e), and SDP₂ ^(e). The offset errors for x₁, x₂, and x₃ are represented by E₁, E₂, and E₃, respectively. Offset errors arise in SDP because SDP is derived from three different interferometer measurements where each of the three interferometers can only measure relative changes in a respective reference and measurement beam paths. In addition, the offset errors may change with time because the calibrations of each of the three interferometers may change with respect to each other, e.g. due to changes in temperature. The effects of changes in the orientation of the stage during the measurements of SDP, SDP₁ ^(e), and SDP₂ ^(e) are accommodated by representing the orientation of the stage l_(z), as l_(z)(y).

The representations of SDP, SDP₁ ^(e) using Equation 11, and SDP₂ ^(e) using Equation 12, that include the effects of offset errors and changes in stage orientation are accordingly expressed as $\begin{matrix} {{{{SDP}\left( {x,y,\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}\left\lbrack {{{\cos\left( {m\quad 2\quad\pi\frac{y}{L}} \right)}A_{m}^{\prime}} + {{\sin\left( {m\quad 2\quad\pi\frac{y}{L}} \right)}B_{m}^{\prime}}} \right\rbrack}} - {x\quad{\overset{\_}{\vartheta}}_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}} - \left\lbrack {E_{1} - {\left( {1 + \eta} \right)E_{2}} + {\eta\quad E_{3}}} \right\rbrack}},{{{- {\frac{1}{2}\left\lbrack {1 - {2\left( \frac{\eta}{1 + \eta} \right)\left( \frac{2b_{3}}{L} \right)}} \right\rbrack}} \leq \frac{y}{L} \leq {\frac{1}{2}\left\lbrack {1 - {2\left( \frac{1}{1 + \eta} \right)\left( \frac{2b_{3}}{L} \right)}} \right\rbrack}};}} & (37) \\ {{{{SDP}_{1}^{e}\left( {x,y,\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}\left\lbrack {{{\cos\left( {m\quad 2\quad\pi\quad\frac{y}{L}} \right)}A_{m}^{\prime}} + {{\sin\left( {m\quad 2\quad\pi\frac{y}{L}} \right)}B_{m}^{\prime}}} \right\rbrack}} - {x\quad{\overset{\_}{\vartheta}}_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{1}^{e}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}} - {\left( {1 + {\eta\quad q}} \right)E_{1}} + {\left( {1 + \eta}\quad \right)E_{2}} + {{\eta\left( {q - 1} \right)}E_{3}} + {\eta\left( \frac{{\xi\left( {y_{0} + \frac{L}{2}} \right)} - {\xi\left( {y_{0} - \frac{L}{2}} \right)}}{2} \right)} + {\eta\quad b_{3}\begin{Bmatrix} {{\vartheta_{z}(y)} + {\vartheta_{z}\left( {y - {2b_{3}}} \right)}} \\ {{+ \ldots} + {\vartheta_{z}\left\lbrack {y - {2\left( {q - 1} \right)b_{3}}} \right\rbrack}} \end{Bmatrix}}}},{{{\frac{1}{2}\left\lbrack {1 - {2\left( \frac{1}{1 + \eta} \right)\left( \frac{2b_{3}}{L} \right)}} \right\rbrack} \leq \frac{y}{L} \leq \frac{1}{2}};{and}}} & (38) \\ {{{{SDP}_{2}^{e}\left( {x,y,\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}\left\lbrack {{{\cos\left( {m\quad 2\quad\pi\quad\frac{y}{L}} \right)}A_{m}^{\prime}} + {{\sin\left( {m\quad 2\quad\pi\frac{y}{L}} \right)}B_{m}^{\prime}}} \right\rbrack}} - {x\quad{\overset{\_}{\vartheta}}_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{2}^{e}\left( {y,{\vartheta_{z} = 0}} \right)} \right\rbrack}} + {\left( {q - 1} \right)E_{1}} + {\left( {1 + \eta} \right)E_{2}} - {\left( {q + \eta} \right)E_{3}} - \left( \frac{{\xi\left( {y_{0} + \frac{L}{2}} \right)} - {\xi\left( {y_{0} - \frac{L}{2}} \right)}}{2} \right) + {b_{3}\begin{Bmatrix} {{\vartheta_{z}(y)} + {\vartheta_{z}\left( {y + L - {2b_{3}}} \right)} + {\vartheta_{z}\left( {y + L - {4b_{3}}} \right)}} \\ {{+ \ldots} + {\vartheta_{z}\left\lbrack {y + L - {2\left( {q - 1} \right)b_{3}}} \right\rbrack}} \end{Bmatrix}}}},{{- \frac{1}{2}} \leq \frac{y}{L} \leq {- {\frac{1}{2}\left\lbrack {1 - {2\left( \frac{\eta}{1 + \eta} \right)\left( \frac{2b_{3}}{L} \right)}} \right\rbrack}}}} & (39) \end{matrix}$

where fourth order of effects arising from the y dependence of l_(z)(y) have been neglected in Equations (37), (38), and (39) and {overscore (l)}_(z) represents the average value of l_(z)(y) over the domain in y.

The lower and upper limits y₁ and y₂, respectively, of the domains in y for SDP₁ ^(e), and SDP₂ ^(e), respectively, are $\begin{matrix} {{y_{1} = {y_{0} + \frac{L}{2} - {2\left( {b_{3} - b_{2}} \right)}}},} & (40) \\ {y_{2} = {y_{0} - \frac{L}{2} + {2b_{2}}}} & (41) \end{matrix}$

where y₀ corresponds to the value of y at the middle of the domain in y. At the lower and upper limits y₁ and y₂, the respective SDP₁ ^(e) and SDP₂ ^(e) are expressed as $\begin{matrix} {{{SDP}_{1}^{e}\left( {x,y_{1},\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}\left\lbrack {{{\cos\left( {m\quad 2\quad\pi\frac{y_{1}}{L}} \right)}A_{m}^{\prime}} + {{\sin\left( {m\quad 2\pi\quad\frac{y_{1}}{L}} \right)}B_{m}^{\prime}}} \right\rbrack}} -}} & (42) \\ {{x{\overset{\_}{\quad\vartheta}}_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{1}^{e}\left( {y_{1},{\vartheta_{z} = 0}} \right)} \right\rbrack}} - {\left( {1 + {\eta\quad q}} \right)E_{1}} + {\left( {1 + \eta} \right)E_{2}} +} & \quad \\ {{\eta\left( {q - 1} \right)E_{3}} + {\eta\left( \frac{{\xi\left( {y_{0} + \frac{L}{2}} \right)} - {\xi\left( {y_{0} - \frac{L}{2}} \right)}}{2} \right)} +} & \quad \\ {{\eta\quad b_{3}\begin{Bmatrix} {{\vartheta_{z}\left\lbrack {y_{0} + \frac{L}{2} - {2\left( {b_{3} - b_{2}} \right)}} \right\rbrack} + {\vartheta_{z}\left\lbrack {y_{0} + \frac{L}{2} - {2\left( {b_{3} - b_{2}} \right)} - {2b_{3}}} \right\rbrack}} \\ {{+ \ldots} + {\vartheta_{z}\left\lbrack {y_{0} + \frac{L}{2} - {2\left( {b_{3} - b_{2}} \right)} - {2\left( {q - 1} \right)b_{3}}} \right\rbrack}} \end{Bmatrix}},} & \quad \\ {{{SDP}_{2}^{e}\left( {x,y_{2},\vartheta_{z}} \right)} = {{\frac{1}{2}{\sum\limits_{m = 1}^{N}\left\lbrack {{{\cos\left( {m\quad 2\quad\pi\frac{y_{2}}{L}} \right)}A_{m}^{\prime}} + {{\sin\left( {m\quad 2\pi\quad\frac{y_{2}}{L}} \right)}B_{m}^{\prime}}} \right\rbrack}} -}} & (43) \\ {{x\quad{\overset{\_}{\vartheta}}_{z}{\frac{\partial}{\partial y}\left\lbrack {{SDP}_{2}^{e}\left( {y_{2},{\vartheta_{z} = 0}} \right)} \right\rbrack}} + {\left( {q - 1} \right)E_{1}} +} & \quad \\ {{\left( {1 + \eta} \right)E_{2}} - {\left( {q + \eta} \right)E_{3}} + \left( \frac{{\xi\left( {y_{0} + \frac{L}{2}} \right)} - {\xi\left( {y_{0} - \frac{L}{2}} \right)}}{2} \right) +} & \quad \\ {{b_{3}\begin{Bmatrix} {{\vartheta_{z}\left\lbrack {y_{0} + \frac{L}{2} + {2b_{2}}} \right\rbrack} + {\vartheta_{z}\left\lbrack {y_{0} + \frac{L}{2} + {2b_{2}} - {2b_{3}}} \right\rbrack}} \\ {+ {\vartheta_{z}\left\lbrack {y_{0} + \frac{L}{2} + {2b_{2}} - {4b_{3}}} \right\rbrack}} \\ {{+ \ldots} + {\vartheta_{z}\left\lbrack {y_{0} + \frac{L}{2} + {2b_{2}} - {2\left( {q - 1} \right)b_{3}}} \right\rbrack}} \end{Bmatrix}},} & \quad \end{matrix}$

It is evident on examination of Equations (37), (42), and (43) that the contribution of the surface figure terms to SDP and SDP₁ ^(e) are continuous at y₁ and that the contribution of the surface figure terms to SDP and SDP₂ ^(e) are continuous at y₂. This is a very significant property which is subsequently used in a procedure to eliminate the effects of offset errors E₁, E₂, and E₃ and the effects of the y dependence of l_(z)(y).

As a consequence of the property, the ratio of the differences between SDP and SDP₁ ^(e) at y₁ and between SDP and SDP₂ ^(e) at y₂ is independent of the surface figure except for the values of the surface figure error at the extreme edges of the domain being mapped. Expressions for the differences are obtained using Equations (37), (42), and (43) with the results $\begin{matrix} {\left\lbrack {{{SDP}_{1}^{e}\left( {x,y_{1},\vartheta_{z}} \right)} - {{SDP}\left( y_{1} \right)}} \right\rbrack = {{{- \eta}\quad{q\left( {E_{1} - E_{3}} \right)}} + {\eta\left( \frac{{\xi\left( {y_{0} + \frac{L}{2}} \right)} - {\xi\left( {y_{0} - \frac{L}{2}} \right)}}{2} \right)} + {\eta\quad{b_{3}\begin{pmatrix} {{\vartheta_{z}\left( {y_{0} + \frac{L}{2} + {2b_{2}} - {2b_{3}}} \right)} + {\vartheta_{z}\left( {y_{0} + \frac{L}{2} + {2b_{2}} - {4b_{3}}} \right)}} \\ {{+ \ldots} + {\vartheta_{z}\left( {y_{0} + \frac{L}{2} + {2b_{2}} - {2{qb}_{3}}} \right)}} \end{pmatrix}}}}} & (44) \\ {\left\lbrack {{{SDP}\left( y_{2} \right)} - {{SDP}_{2}^{e}\left( {x,y_{2},\vartheta_{z}} \right)} -} \right\rbrack = {{- {q\left( {E_{1} - E_{3}} \right)}} + \left( \frac{{\xi\left( {y_{0} + \frac{L}{2}} \right)} - {\xi\left( {y_{0} - \frac{L}{2}} \right)}}{2} \right) + {b_{3}{\quad\begin{pmatrix} {{\vartheta_{z}\left( {y_{0} + \frac{L}{2} + {2b_{2}}} \right)} + {\vartheta_{z}\left( {y_{0} + \frac{L}{2} + {2b_{2}} - {2b_{3}}} \right)}} \\ \begin{matrix} {{+ {\vartheta_{z}\left( {y_{0} + \frac{L}{2} + {2b_{2}} - {4b_{3}}} \right)}} + \ldots +} \\ {\vartheta_{z}\left\lbrack {y_{0} + \frac{L}{2} + {2b_{2}} - {2\left( {q - 1} \right)b_{3}}} \right\rbrack} \end{matrix} \end{pmatrix}\quad}}}} & (45) \end{matrix}$

Using the relationship L=2qb₃ given by Equation (8), Equation (45) is written as $\begin{matrix} {\left\lbrack {{{SDP}\left( y_{2} \right)} - {{SDP}_{2}^{e}\left( {x,y_{2},\vartheta_{z}} \right)} -} \right\rbrack = {{- {q\left( {E_{1} - E_{3}} \right)}} + \left( \frac{{\xi\left( {y_{0} + \frac{L}{2}} \right)} - {\xi\left( {y_{0} - \frac{L}{2}} \right)}}{2} \right) + {{b_{3}\begin{pmatrix} {{\vartheta_{z}\left( {y_{0} + \frac{L}{2} + {2b_{2}} - {2b_{3}}} \right)} + {\vartheta_{z}\left( {y_{0} + \frac{L}{2} + {2b_{2}} - {4b_{3}}} \right)}} \\ {{+ \ldots} + {\vartheta_{z}\left\lbrack {y_{0} + \frac{L}{2} + {2b_{2}} - {2{qb}_{3}}} \right\rbrack}} \end{pmatrix}}.}}} & (46) \end{matrix}$

The ratio of the value of the discontinuity D₁ (y₀) given Equation (44) and the value of the discontinuity D₂ (y₀) given by Equation (46) is thus equal to η, i.e. D ₁(y ₀)=ηD ₂(y ₀)  (47)

where D ₁(y ₀)≡[SDP ₁ ^(e)(x,y ₁ ,l _(z))−SDP(y ₁ ,l _(z))],  (48) D ₂(y ₀)[SDP(y ₂ ,l _(z))−SDP ₂ ^(e)(x,y ₂ ,l _(z))].  (49)

Based on the foregoing mathematical development, a general procedure for determining a surface figure function, ξ(y), without any prior knowledge of the surface is 5 figure is as follows. first, select the length of the mirror that is to be mapped by selecting a value of q. The length of the mirror is given by Equation (8). Orient the stage mirror so that η_(z) is at or about zero and the distance x from the interferometer to the stage mirror being mapped is relatively small. The small distance can reduce the contribution to the geometric error correction term. While maintaining a nominal x distance to the stage mirror, acquire simultaneous values for x₁, x₂, and x₃ while scanning the mirror in the y-direction and monitor the position of the mirror in the y-direction and changes in stage orientation during the scan. The x₁, x₂, and x₃ values, the position of the mirror in the y-direction, and the changes in stage orientation can be stored to the electronic controller's memory or to disk. The stored data will be in the form of a 3×N array for the x₁, x₂, and x₃ information, where N is the total number of samples across the mirror, a 1×N array for y position information and a 1×N array for changes in stage orientation information.

Next, calculate values for SDP, SDP₁ ^(e), and SDP₂ ^(e) on a sampling grid (e.g., a uniform sampling grid) in preparation for a discrete Fourier transform which will be performed later. These calculations can include averaging multiple values of SDP, SDP₁ ^(e), and SDP₂ ^(e) where each increment in the sampling grid corresponds to multiple values of x₁, x₂, and x₃. Since the SDP₁ ^(e), and SDP₂ ^(e) parameters are sensitive to changes in stage orientation during the scan, the array containing changes in stage orientation information during the scan is used to correct the SDP₁ ^(e) and SDP₂ ^(e) parameters to a chosen reference stage orientation.

Next, remove the discontinuities at the domain boundaries between SDP₁ ^(e) and SDP, and between SDP and SDP₂ ^(e) by adding appropriate constant values to SDP₁ ^(e) and SDP₂ ^(e). These constant values are −D₁ and D₂ as given by Equations (48) and (49).

After the discontinuities have been removed, a resultant SDP array is constructed by concatenating the SDP₂ ^(e) array with discontinuity subtracted, SDP array and SDP₁ ^(e) array with discontinuity subtracted. The resultant SDP array spans the length of the mirror to be mapped, L. Next, perform a discrete Fourier transform on the resultant SDP array. Using a complex transfer function calculated for the interferometer being used, transform the SDP Fourier coefficients into the Fourier coefficients for the surface figure function ξ(y). The surface figure function, ξ(y), can now be determined from the Fourier coefficients using Equation (13).

In certain embodiments, as discussed earlier, the interferometer axes spacing can be selected so that the double pass displacement measurements x₁, x₂, and x₃ measured by the interferometer have reduced or nominally zero sensitivity to spatial frequency components corresponding to zeros of the transfer function T(m). In embodiments where manufacturing tolerances or other constraints do not allow this interferometer axes spacing, the contributions of the surface figure error function to the double pass distances x₁, x₂, and x₃ at the spatial frequencies for which the transfer function T(m) is significantly reduced or zero are subsequently measured by alignment wafer procedures that are based on measurements of properties of an alignment wafer. The properties of transfer function T(m) are calculated using a measured value of η and yield in particular the values of the spatial frequencies for which the transfer function T(m) is significantly reduced or zero.

The alignment wafer used in the alignment wafer procedures is generated with a linear array of alignment marks 62 such as shown diagrammatically in FIG. 4. The length of the linear array corresponds to the length of the scan in the y direction for which information about the surface figure is being determined and is represented as L_(a). In some embodiments, L_(a) is in a range from about 10 cm to about 100 cm (e.g., about 20 cm or more, about 30 cm or more up to about 80 cm). The spacing of contiguous alignment marks is d_(a) which corresponds to a spatial frequency 1/d_(a) that is 4 times a harmonic of a spatial frequency for which additional information about the surface figure is desired. The harmonic may be the first harmonic of the spatial frequency if there are no significant effects of aliasing of higher harmonics in subsequent data processing.

In some embodiments, the positions of the alignment marks arranged nominally parallel to the stage mirror are first measured in the x direction by one or more of the three interferometers using an alignment sensor to locate the alignment marks. Next, the linear array of alignment marks is shifted relative to the stage mirror by d_(a) in a direction parallel to the stage mirror and the positions of the alignment marks are measured a second time by the one or more of the three interferometers.

The selected value of the shift d_(a) corresponds to a π/2 phase shift in the conjugated quadrature of a spatial frequency component of the surface figure having a spatial wavelength of Λ=4d_(a). As a consequence of the π/2 phase shift, the difference of the two measurements of the alignment mark positions in the x direction for each of the one or more of the three interferometer axes contains to a high degree of accuracy only the contribution of the spatial frequency components of the surface figure, i.e. the effects of departures of the positions of the array of alignment marks from a datum line cancel out. In addition, the relative sensitivity of the difference of the two measurements to the contribution of the spatial frequency components with spatial wavelength Λ is of the order of ½.

The difference of the two measurements for each of the one or more of the three interferometer axes are analyzed for the Fourier series coefficients for the spatial frequency component having the spatial wavelength Λ. The resulting Fourier series coefficients correspond to the respective spectral component of the surface figure with spatial wavelength Λ.

Without wishing to be bound by theory, a formal description of the first alignment wafer procedure is next presented. The first array of measured locations of the linear array of alignment marks is represented by x_(i)(y_(j)) for i=1, 2, and/or 3 where y_(j) corresponds to the location in the y direction of alignment mark j where 1≦j≦N_(a). The number of alignment marks, N_(a), is related to the scan length L_(a) in the y direction as $\begin{matrix} {N_{a} = {4{\frac{L_{a}}{\Lambda}.}}} & (50) \end{matrix}$

Note that N_(a) is an even integer mod 4. The second array of measured locations of the linear array of alignment marks is represented by x_(i)(y_(j)+d_(a)) for i=1, 2, and/or 3. The difference of the two arrays may be expressed as $\begin{matrix} {{\left\lbrack {{x_{i}\left( {y_{j} + d_{a}} \right)} - {x_{i}\left( y_{j} \right)}} \right\rbrack = {{\sum\limits_{m = 1}^{N}{{\overset{\sim}{A}}_{m}\left\{ {{\cos\left\lbrack {m\quad 2\pi\frac{\left( {y_{j} + d_{a}} \right)}{L_{a}}} \right\rbrack} - {\cos\left( {m\quad 2\quad\pi\frac{y_{j}}{L_{a}}} \right)}} \right\}}} + {\sum\limits_{m = 1}^{N}{{\overset{\sim}{B}}_{m}\left\{ {{\sin\left\lbrack {m\quad 2\pi\frac{\left( {y_{j} + d_{a}} \right)}{L_{a}}} \right\rbrack} - {\sin\left( {m\quad 2\quad\pi\quad\frac{y_{j}}{L_{a}}} \right)}} \right\}}} + \overset{\_}{x} + {\Delta\quad{\overset{\_}{\vartheta}}_{z}{d_{a}\left( {j - 1} \right)}}}},{1 \leq j \leq N_{a}},} & (51) \end{matrix}$ where {overscore (x)} is the shift in the x direction of alignment mark j=1 and Δ{overscore (l)}_(z), is the change in the orientation of the alignment wafer, respectively, that are introduced when the alignment wafer is shifted in the y direction by d_(a) and Ã_(m) and {tilde over (B)}_(m) are the respective Fourier coefficients corresponding to the specific double pass measurement indicated by the index i. It is important to note that the Ã_(m) and {tilde over (B)}_(m) Fourier coefficients utilized here represent the contributions of the mirror surface figure error function to the double pass displacement measurements and thus do not correspond directly to the Fourier coefficients of the surface figure error function found in Equation (13). Equation (51) is rewritten using trigonometric identities as $\begin{matrix} {{\left\lbrack {{x_{i}\left( {y_{j} + d_{a}} \right)} - {x_{i}\left( y_{j} \right)}} \right\rbrack = {{\sum\limits_{m = 1}^{N}{\begin{Bmatrix} {{{\overset{\sim}{A}}_{m}\left\lbrack {{\cos\left( {m\quad 2\quad\pi\frac{d_{a}}{L_{a}}} \right)} - 1} \right\rbrack} +} \\ {{\overset{\sim}{B}}_{m}{\sin\left( {m\quad 2\quad\pi\frac{d_{a}}{L_{a}}} \right)}} \end{Bmatrix}{\cos\left\lbrack {m\quad 2\quad\pi\frac{y_{j}}{L_{a}}} \right\rbrack}}} + {\sum\limits_{m = 1}^{N}{\begin{Bmatrix} {{{- {\overset{\sim}{A}}_{m}}{\sin\left( {m\quad 2\quad\pi\frac{d_{a}}{L_{a}}} \right)}} +} \\ {{\overset{\sim}{B}}_{m}\left\lbrack {{\cos\left( {m\quad 2\quad\pi\frac{d_{a}}{L_{a}}} \right)} - 1} \right\rbrack} \end{Bmatrix}{\sin\left( {m\quad 2\quad\pi\frac{y_{j}}{L_{a}}} \right)}}} + \overset{\_}{x} + {\Delta{\overset{\_}{\vartheta}}_{z}{d_{a}\left( {j - 1} \right)}}}},{1 \leq j \leq {N_{a}.}}} & (52) \end{matrix}$

Using the orthogonality properties of the trigonometric functions, the following Fourier coefficients are obtained to a good approximation as $\begin{matrix} {{\left( {{\overset{\sim}{A}}_{m^{\prime}} - {\overset{\sim}{B}}_{m^{\prime}}} \right) = {{- \left\{ {\frac{2}{N_{a}}{\sum\limits_{j = 1}^{N_{a}}{\left\lbrack {{x_{i}\left( {y_{j} + d_{a}} \right)} - {x_{i}\left( y_{j} \right)}} \right\rbrack{\cos\left\lbrack {m^{\prime}2\quad\pi\frac{y_{j}}{L_{a}}} \right\rbrack}}}} \right\}}{\delta\left( {m^{\prime} - {N_{a}/4}} \right)}}},} & (53) \\ {{\left( {{\overset{\sim}{A}}_{m^{\prime}} + {\overset{\sim}{B}}_{m^{\prime}}} \right) = {{{- \left\{ {\frac{2}{N_{a}}{\sum\limits_{j = 1}^{N_{a}}{\left\lbrack {{x_{i}\left( {y_{j} + d_{a}} \right)} - {x_{i}\left( y_{j} \right)}} \right\rbrack{\sin\left\lbrack {m^{\prime}2\quad\pi\frac{y_{j}}{L_{a}}} \right\rbrack}}}} \right\}}{\delta\left( {m^{\prime} - {N_{a}/4}} \right)}} - {\Delta{\overset{\_}{\vartheta}}_{z}d_{a}}}},} & (54) \end{matrix}$ where δ(m) is the Kronecker delta function, i.e. δ(m)=1, m=0 and δ(m)=0, m≠0. Ã_(m), and {tilde over (B)}_(m), as indicated here correspond to the specific double pass measurement indicated by the index i, and thus values of Ã_(m), and {tilde over (B)}_(m), must be calculated separately for each of the double pass measurements for which a surface figure error correction corresponding to the spatial frequency $\frac{N_{a}}{4L_{a}}$ is desired. The value of the constant term Δ{overscore (l)}_(z)d_(a) in Equation (54) is determined from the product of Δ{overscore (l)}_(z) obtained from a linear fit to the difference [x_(i)(y_(j)+d_(a))−x_(i)(y_(j))] and d_(a) obtained from the measured positions of the alignment marks in the y direction. With the determined value of Δ{overscore (l)}_(z)d_(a), values for Ã_(m′) and {tilde over (B)}_(m′) for m′=N_(a)/4 are obtained from Equations (53) and (54).

The coefficients Ã_(m′) and {tilde over (B)}_(m′) as obtained can then be used to generate corrections for the corresponding double pass measurement for those components of the surface figure error function having spatial frequency $\frac{N_{a}}{4L_{a}}.$

The effects of aliasing have been omitted, for example, in Equations (53) and (54)

In embodiments, the effects of aliasing can be evaluated in an end use application by repeating the steps of the alignment wafer procedure with an alignment wafer that has a d_(a) corresponding to ¼ of the spatial wavelength of the spectral component responsible for the undesired aliased component.

In certain embodiments, the positions of the alignment marks arranged nominally parallel to the stage mirror are first measured in the x direction by one or more of the three interferometers. Next, the alignment wafer is rotated by 180 degrees and the positions of the alignment marks are measured a second time.

For the analysis in such embodiments, the measured position of an alignment mark from the first measurement is added with the measured position of a conjugate alignment mark from the second measurement wherein an alignment mark and its conjugate alignment mark have the same nominal position in the y direction. The analysis for data acquired in such procedures is the same as the analysis described above.

In some embodiments, this alignment wafer procedure can be used to determine surface figures for mirrors in a lithography tool at times when the tool is not being used to expose wafers. For example, this procedure can be used during routine maintenance of the tool. At such times, a dedicated scan sequence can be implemented, allowing a portion of a mirror to be scanned at a rate optimized for mirror characterization purposes. Moreover, multiple scans can be performed for different relative distances between the mirror and the interferometer and at different nominal stage orientations, providing a family of ultimate surface figures which can be interpolated for use at other relative distances between the mirror and the interferometer and at other stage orientations.

In embodiments where data is acquired during dedicated scan sequences, the data can be acquired over time periods that are relatively long with respect to various sources of random errors in x₁, x₂, and x₃ measurements. Accordingly, uncertainty in surface figures due to random errors sources can be reduced. For example, one source of random errors are fluctuations in the composition or density of the atmosphere in the interferometer beam paths. Over relatively long time periods, these fluctuations average to zero. Accordingly, acquiring data for calculating SDP and SDP^(e) values over sufficiently long periods can substantially reduce the uncertainty of ξ(y) due to these non-stationary atmospheric fluctuations.

In certain embodiments where the mirror is to be mapped in situ during, for example, lithography tool operation, arrays of x₁, x₂, and x₃, y position and stage orientation can be acquired and stored to the electronic controller's memory or to disk for specific relative distances and nominal stage orientations. After the arrays of data have been acquired, the remaining steps for mapping the surface figure are the same as in an offline analysis. Values for SDP, SDP₁ ^(e), and SDP₂ ^(e) can be calculated and assigned to a sampling grid (e.g., a uniform sampling grid) in preparation for a discrete Fourier transform which will be performed later. These calculations can include averaging multiple values of SDP, SDP₁ ^(e), and SDP₂ ^(e) where each increment in the sampling grid corresponds to multiple values of x₁, x₂, and x₃. Since the SDP₁ ^(e), and SDP₂ ^(e) parameters are sensitive to changes in stage orientation during the scan, the array containing changes in stage orientation information during the scan is used to correct the SDP₁ ^(e) and SDP₂ ^(e) parameters to a chosen reference stage orientation.

Next, the discontinuities at the domain boundaries between SDP₁ ^(e) and SDP, and between SDP and SDP ₂ ^(e) are removed by adding appropriate constant values to SDP₁ ^(e) and SDP₂ ^(e). These constant values are −D₁ and D₂ as given by Equations (48) and (49).

After the discontinuities have been removed, a resultant SDP array is constructed by appropriately concatenating the SDP₂ ^(e), SDP and SDP₁ ^(e) arrays. The resultant SDP array spans the length of the mirror to be mapped, L. Next, perform a discrete Fourier transform on the resultant SDP array. Using a complex transfer function calculated for the interferometer being used, transform the SDP Fourier coefficients into the Fourier coefficients for the surface figure function ξ(y). The surface figure function, ξ(y), can now be determined from the Fourier coefficients using Equation (13).

The surface figure function may be updated and maintained by computing a running average of the surface figure function acquired at successive time intervals. The running average can be stored to the electronic controller's memory or to disk. The optimum time interval which a given average spans can be chosen after determining the time scales over which the surface figure function ξ(y) significantly changes.

In certain other embodiments, a predetermined surface figure function ξ can be updated or variations in ξ can be monitored based on values of SDP and/or SDP^(e)s calculated from newly-acquired interferometry data. For example, in a lithography tool, x₁, x₂, and x₃ values acquired during operation of the tool (e.g., during wafer exposure) can be used to update a mirror's surface figure, or can be used to monitor changes in the surface figure and provide an indicator of when new full mirror characterizations are required to maintain the interferometry system's accuracy.

In implementations where the surface figure function is updated during an exposure sequence of a tool, data can be acquired over multiple wafer exposure sequences so that changes that occur to the surface figure function as a result of systematic changes in the tool that occur each sequence can be distinguished from actual permanent changes in the mirror's characteristics. One example of systematic changes in a tool that may contribute to variations in a surface figure function are stationary changes in the atmosphere in the interferometer's beam paths. Such changes occur for each wafer exposure cycle as the composition and/or gas pressure inside the lithography tool is changed. In the absence of any other technique for monitoring and/or compensating for these effects, they can result in errors in the x₁, x₂, and x₃ measurements that ultimately manifest as errors in the surface figure function. However, since the changes to the atmosphere are stationary, their effect on ξ(y) can be reduced (e.g., eliminated) by identifying variations that occur to ξ(y) with the same period as the wafer exposure cycle, and subtracting these variations from the correction that is ultimately made to a stage measurement.

The predetermined surface figure function in the certain other embodiments may be updated by creating a running average of the surface figure function using the predetermined surface figure function and surface figure functions acquired in situ at subsequent time intervals. The subsequent surface figure functions acquired in situ may be acquired as in the certain embodiments description above. The running average can be stored to the electronic controller's memory or to disk. The optimum time interval which a given average spans can be chosen after determining the time scales over which the surface figure function ξ(y) significantly changes.

An alternative procedure for updating a predetermined surface figure in the certain other embodiments above may be used. The first step in the alternate procedure is to measure values of SDP(y, {overscore (l)}_(z)=0) for a section of the x-axis stage mirror. The length of the section or domain is ≧4b₃ and can include the entire length of the stage mirror. Next, integrals of SDP(y, {overscore (l)}_(z)=0) with weight functions cos(s2πy/L) and sin (s2πy/L) are computed from the measured values of SDP(y,{overscore (l)}_(z)=0) minus the mean value <SDP (y,{overscore (l)}_(z)=0)> of SDP (y,{overscore (l)}_(z)=0), SDP(y,{overscore (l)}_(z)=0)−ηD(y₀), and SDP₂ ^(e) (y, {overscore (l)}_(z)=0)+D(y₀), <SDP(y, {overscore (l)}_(z)=0)≦. The integrals are: $\begin{matrix} {{A_{s}^{''} = {\frac{4}{\left( {L - {2b_{3}}} \right)} \times {\int_{({{- \frac{L}{2}} + {2b_{2}}})}^{\lbrack{\frac{L}{2} - {2{({b_{3} - b_{2}})}}}\rbrack}{\left\lbrack {{{SDP}\left( {y,{{\overset{\_}{\vartheta}}_{z} = 0}} \right)} - \left\langle {{SDP}\left( {y,{{\overset{\_}{\vartheta}}_{z} = 0}} \right)} \right\rangle} \right\rbrack{\sin\left( \frac{s\quad 2\pi\quad y}{L} \right)}\quad{\mathbb{d}y}}}}},{s \geq 1},} & (52) \\ {{B_{s}^{''} = {\frac{4}{\left( {L - {2b_{3}}} \right)} \times {\int_{({{- \frac{L}{2}} + {2b_{2}}})}^{\lbrack{\frac{L}{2} - {2{({b_{3} - b_{2}})}}}\rbrack}{\left\lbrack {{{SDP}\left( {y,{{\overset{\_}{\vartheta}}_{z} = 0}} \right)} - \left\langle {{SDP}\left( {y,{{\overset{\_}{\vartheta}}_{z} = 0}} \right)} \right\rangle} \right\rbrack{\sin\left( \frac{s\quad 2\pi\quad y}{L} \right)}\quad{\mathbb{d}y}}}}},{s \geq 1.}} & (53) \end{matrix}$

The integrals expressed by Equations (52) and (53) are evaluated using the series representation of SDP given by Equation (16) with the results $\begin{matrix} {{A_{q}^{''} = {\frac{4}{\left( {L - {2b_{3}}} \right)} \times {\int_{({{- \frac{L}{2}} + {2b_{2}}})}^{\lbrack{\frac{L}{2} - {2{({b_{3} - b_{2}})}}}\rbrack}{\begin{bmatrix} {{\sum\limits_{m = 1}^{N}{A_{m}^{\prime}{\cos\left( \frac{m\quad 2\pi\quad y}{L} \right)}{\cos\left( \frac{q\quad 2\pi\quad y}{L} \right)}}} +} \\ {\sum\limits_{m = 1}^{N}{B_{m}^{\prime}{\sin\left( \frac{m\quad 2\pi\quad y}{L} \right)}{\cos\left( \frac{q\quad 2\pi\quad y}{L} \right)}}} \end{bmatrix}\quad{\mathbb{d}y}}}}},{q \geq 1},} & (54) \\ {B_{q}^{''} = {{\frac{4}{\left( {L - {2\quad b_{3}}} \right)} \times {\int_{{({{- \frac{L}{2}}\quad + {2\quad b_{2}}})}\quad}^{\lbrack{\frac{L}{2} - {2\quad{({b_{3} - b_{2}})}}}\rbrack}{\begin{bmatrix} {{\sum\limits_{m = 1}^{N}{{\quad A_{m}^{\prime}}\quad{\cos\left( \frac{m\quad 2\quad\pi\quad y}{L} \right)}\quad{\sin\left( \frac{q\quad 2\quad\pi\quad y}{L} \right)}}} +} \\ {\sum\limits_{m = 1}^{N}{{\quad B_{m}^{\prime}}\quad{\sin\left( \frac{m\quad 2\quad\pi\quad y}{L} \right)}\quad{\sin\left( \frac{q\quad 2\quad\pi\quad y}{L} \right)}}} \end{bmatrix}\quad{\mathbb{d}y}\quad q}}} \geq 1.}} & (55) \end{matrix}$

where coefficients A_(q)′ and B_(q)′ are with respect to SDP(y,{overscore (l)}_(z)=0) with <SDP(y,{overscore (l)}_(z)=0)> subtracted. The evaluation of the integrals in Equation (54) is next performed with the results $\begin{matrix} {{A_{q}^{''} = {\frac{1}{\left( {1 - \frac{2b_{3}}{L}} \right)} \times \begin{Bmatrix} {{\sum\limits_{m = 1}^{N}{A_{m}^{\prime}\left( \begin{pmatrix} {{\frac{1}{\left( {q + m} \right)2\pi}\begin{Bmatrix} {{\sin\quad{{\pi\left( {q + m} \right)}\left\lbrack {1 - {4\frac{\left( {b_{3} - b_{2}} \right)}{L}}} \right\rbrack}} +} \\ {\sin\quad{{\pi\left( {q + m} \right)}\left\lbrack {1 - {4\frac{b_{2}}{L}}} \right\rbrack}} \end{Bmatrix}} +} \\ {\frac{1}{\left( {q - m} \right)2\pi}\begin{Bmatrix} {{\sin\quad{{\pi\left( {q - m} \right)}\left\lbrack {1 - {4\frac{\left( {b_{3} - b_{2}} \right)}{L}}} \right\rbrack}} +} \\ {\sin\quad{{\pi\left( {q - m} \right)}\left\lbrack {1 - {4\frac{b_{2}}{L}}} \right\rbrack}} \end{Bmatrix}} \end{pmatrix} \right)}} -} \\ {\sum\limits_{m = 1}^{N}{B_{m}^{\prime}\left( \begin{pmatrix} {{\frac{1}{\left( {q + m} \right)2\pi}\begin{Bmatrix} {{\cos\quad{{\pi\left( {q + m} \right)}\left\lbrack {1 - {4\frac{\left( {b_{3} - b_{2}} \right)}{L}}} \right\rbrack}} -} \\ {\cos\quad{{\pi\left( {q + m} \right)}\left\lbrack {1 - {4\frac{b_{2}}{L}}} \right\rbrack}} \end{Bmatrix}} -} \\ {\frac{1}{\left( {q - m} \right)2\pi}\begin{Bmatrix} {{\cos\quad{{\pi\left( {q - m} \right)}\left\lbrack {1 - {4\frac{\left( {b_{3} - b_{2}} \right)}{L}}} \right\rbrack}} -} \\ {\cos\quad{{\pi\left( {q - m} \right)}\left\lbrack {1 - {4\frac{b_{2}}{L}}} \right\rbrack}} \end{Bmatrix}} \end{pmatrix} \right)}} \end{Bmatrix}}},{q \geq 1},} & (56) \\ {{{A_{q}^{''} = {A_{q}^{\prime} + {\frac{1}{\left( {1\quad - \frac{2\quad b_{3}}{L}} \right)} \times \begin{Bmatrix} {{\underset{m \neq q}{\sum\limits_{{m = 1},}^{N}}{A_{m}^{\prime}\left( \begin{pmatrix} {{\frac{\left( {- 1} \right)^{q + m + 1}}{\left( {q + m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\sin\quad{{\pi\left( {q + m} \right)}\left\lbrack {4\quad\frac{\left( {b_{3} - b_{2}} \right)}{L}} \right\rbrack}} +} \\ {\sin\quad{\pi\left( {q + m} \right)}\left( {4\quad\frac{b_{2}}{L}} \right)} \end{Bmatrix}} +} \\ {\frac{\left( {- 1} \right)^{q - m + 1}}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\sin\quad{{\pi\left( {q - m} \right)}\left\lbrack {4\quad\frac{\left( {b_{3} - b_{2}} \right)}{L}} \right\rbrack}} +} \\ {{\sin\quad{\pi\left( {q - m} \right)}\left( {4\quad\frac{b_{2}}{L}} \right)}\quad} \end{Bmatrix}} \end{pmatrix} \right)}} -} \\ {\sum\limits_{m = 1}^{N}{B_{m}^{\prime}\left( \begin{pmatrix} {{\frac{\left( {- 1} \right)^{q - m}}{\left( {q + m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\quad{{\pi\left( {q + m} \right)}\left\lbrack {4\quad\frac{\left( {b_{3} - b_{2}} \right)}{L}} \right\rbrack}} -} \\ {{\cos\quad{{\pi\left( {q + m} \right)}\left\lbrack {4\quad\frac{b_{2}}{L}} \right\rbrack}}\quad} \end{Bmatrix}} -} \\ {\frac{\left( {- 1} \right)^{q - m}}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\quad{{\pi\left( {q - m} \right)}\left\lbrack \quad{4\quad\frac{\left( {b_{3} - b_{2}} \right)}{L}} \right\rbrack}} -} \\ {\cos\quad{\pi\left( {q - m} \right)}\left( {4\frac{b_{2}}{L}} \right)} \end{Bmatrix}} \end{pmatrix} \right)}} \end{Bmatrix}}}},{q \geq 1},}\quad} & (57) \\ {{{A_{q}^{''} = {A_{q}^{\prime} + {\frac{1}{\left( {1 - \frac{2\quad b_{3}}{L}} \right)} \times \left\{ \begin{matrix} {{\underset{m \neq q}{\sum\limits_{{m = 1},}^{N}}{A_{m}^{\prime}\left( \begin{pmatrix} {{\frac{\left( {- 1} \right)^{q + m + 1}}{\left( {q + m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\sin\quad\left\lbrack {2{\pi\left( {q + m} \right)}\quad\frac{1}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} +} \\ {\sin\quad\left\lbrack {2{\pi\left( {q + m} \right)}\quad\frac{\eta}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} +} \\ {\frac{\left( {- 1} \right)^{q - m + 1}}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\sin\left\lbrack {2\quad{\pi\left( {q - m} \right)}\frac{1}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} +} \\ {\sin\left\lbrack {2\quad{\pi\left( {q - m} \right)}\frac{\eta}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} \end{pmatrix} \right)}} -} \\ {\sum\limits_{m = 1}^{N}{B_{m}^{\prime}\left( \begin{pmatrix} {{\frac{\left( {- 1} \right)^{q - m}}{\left( {q + m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\left\lbrack {2{\pi\left( {q + m} \right)}\quad\frac{1}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} -} \\ {\cos\left\lbrack {2{\pi\left( {q + m} \right)}\quad\frac{\eta}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} -} \\ {\frac{\left( {- 1} \right)^{q - m}}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\left\lbrack {2\quad{\pi\left( {q - m} \right)}\frac{1}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} -} \\ {\cos\left\lbrack {2\quad{\pi\left( {q - m} \right)}\frac{\eta}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} \end{pmatrix} \right)}} \end{matrix}\quad \right\}}}}\quad,{q \geq 1},}\quad} & (58) \\ {{{A_{q}^{''} = {A_{q}^{\prime} + {\frac{\left( \frac{2b_{3}}{L} \right)}{\left\lbrack {1 - \left( \frac{2\quad b_{3}}{L} \right)} \right\rbrack} \times \left\{ \begin{matrix} {{\underset{m \neq q}{\sum\limits_{{m = 1},}^{N}}{A_{m}^{\prime}\left( \begin{pmatrix} {{\left( {- 1} \right)^{q + m + 1}\begin{Bmatrix} {\sin\quad{c\quad\left\lbrack {{\pi\left( {q + m} \right)}\quad\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \times} \\ {\cos\left\lbrack {{\pi\left( {q + m} \right)}\quad\frac{\left( {\eta - 1} \right)}{\left( {\eta + 1} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} +} \\ {\left( {- 1} \right)^{q - m + 1}\begin{Bmatrix} {\sin\quad{c\left\lbrack {{\pi\left( {q - m} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \times} \\ {\cos\left\lbrack \quad{{\pi\left( {q - m} \right)}\frac{\left( {\eta - 1} \right)}{\left( {\eta + 1} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} \end{pmatrix} \right)}} +} \\ {\sum\limits_{m = 1}^{N}{B_{m}^{\prime}\left( \begin{pmatrix} {{\left( {- 1} \right)^{q - m + 1}\begin{Bmatrix} {\sin\quad{c\left\lbrack {{\pi\left( {q + m} \right)}\quad\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \times} \\ {\sin\left\lbrack {{\pi\left( {q + m} \right)}\quad\frac{\left( {\eta - 1} \right)}{\left( {\eta + 1} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} -} \\ {\left( {- 1} \right)^{q - m + 1}\begin{Bmatrix} {\sin\quad{c\left\lbrack {{\pi\left( {q - m} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \times} \\ {\sin\left\lbrack {{\pi\left( {q - m} \right)}\frac{\left( {\eta - 1} \right)}{\left( {\eta + 1} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} \end{pmatrix} \right)}} \end{matrix}\quad \right\}}}},{q \geq 1.}}\quad} & (59) \end{matrix}$

The evaluation of the integrals in Equation (55) is next performed with the results $\begin{matrix} {{{B_{q}^{''} = {\frac{1}{\left( {1 - \frac{2\quad b_{3}}{L}} \right)} \times \left\{ \begin{matrix} {{- {\sum\limits_{m = 1}^{N}{A_{m}^{\prime}\left( \begin{pmatrix} {{\frac{1}{\left( {q + m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\quad{{\pi\left( {q + m} \right)}\quad\left\lbrack {1 - {4\frac{\left( {b_{3} - b_{2}} \right)}{L}}} \right\rbrack}} -} \\ {\cos\quad{{\pi\left( {q + m} \right)}\quad\left\lbrack {1 - {4\frac{b_{2}}{L}}} \right\rbrack}} \end{Bmatrix}} +} \\ {\frac{1}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\quad{{\pi\left( {q - m} \right)}\left\lbrack {1 - {4\frac{\left( {b_{3} - b_{2}} \right)}{L}}} \right\rbrack}} -} \\ {\cos\quad{{\pi\left( {q - m} \right)}\left\lbrack {1 - {4\frac{b_{2}}{L}}} \right\rbrack}} \end{Bmatrix}} \end{pmatrix} \right)}}} +} \\ {\sum\limits_{m = 1}^{N}{B_{m}^{\prime}\left( \begin{pmatrix} {{\frac{1}{\left( {q + m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\sin\quad{{\pi\left( {q + m} \right)}\quad\left\lbrack {1 - {4\frac{\left( {b_{3} - b_{2}} \right)}{L}}} \right\rbrack}} +} \\ {\sin\quad{{\pi\left( {q + m} \right)}\quad\left\lbrack {1 - {4\frac{b_{2}}{L}}} \right\rbrack}} \end{Bmatrix}} +} \\ {\frac{1}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\sin\quad{{\pi\left( {q - m} \right)}\left\lbrack {1 - {4\frac{\left( {b_{3} - b_{2}} \right)}{L}}} \right\rbrack}} +} \\ {\sin\quad{{\pi\left( {q - m} \right)}\left\lbrack {1 - {4\frac{b_{2}}{L}}} \right\rbrack}} \end{Bmatrix}} \end{pmatrix} \right)}} \end{matrix}\quad \right\}}}\quad,{q \geq 1},}\quad} & (60) \\ {{{B_{q}^{''} = {B_{q}^{\prime} + {\frac{1}{\left( {1 - \frac{2\quad b_{3}}{L}} \right)} \times \left\{ \begin{matrix} {{- {\sum\limits_{m = 1}^{N}{A_{m}^{\prime}\left( \begin{pmatrix} {{\frac{\left( {- 1} \right)^{q + m}}{\left( {q + m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\quad{{\pi\left( {q + m} \right)}\quad\left\lbrack {4\frac{\left( {b_{3} - b_{2}} \right)}{L}} \right\rbrack}} -} \\ {\cos\quad{{\pi\left( {q + m} \right)}\quad\left\lbrack {4\frac{b_{2}}{L}} \right\rbrack}} \end{Bmatrix}} +} \\ {\frac{\left( {- 1} \right)^{q - m}}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\quad{{\pi\left( {q - m} \right)}\left\lbrack {4\frac{\left( {b_{3} - b_{2}} \right)}{L}} \right\rbrack}} -} \\ {\cos\quad{\pi\left( {q - m} \right)}\left( {4\frac{b_{2}}{L}} \right)} \end{Bmatrix}} \end{pmatrix} \right)}}} +} \\ {\underset{m \neq q}{\sum\limits_{m = 1}^{N}}{B_{m}^{\prime}\left( \begin{pmatrix} {{{- \frac{\left( {- 1} \right)^{q + m + 1}}{\left( {q + m} \right)\quad 2\quad\pi}}\begin{Bmatrix} {{\sin\quad{{\pi\left( {q + m} \right)}\quad\left\lbrack {4\frac{\left( {b_{3} - b_{2}} \right)}{L}} \right\rbrack}} +} \\ {\sin\quad{\pi\left( {q + m} \right)}\quad\left( {4\frac{b_{2}}{L}} \right)} \end{Bmatrix}} +} \\ {\frac{\left( {- 1} \right)^{q - m + 1}}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\sin\quad{{\pi\left( {q - m} \right)}\left\lbrack {4\frac{\left( {b_{3} - b_{2}} \right)}{L}} \right\rbrack}} +} \\ {\sin\quad{\pi\left( {q - m} \right)}\left( {4\frac{b_{2}}{L}} \right)} \end{Bmatrix}} \end{pmatrix} \right)}} \end{matrix}\quad \right\}}}}\quad,{q \geq 1},}\quad} & (61) \\ {{{B_{q}^{''} = {B_{q}^{\prime} + {\frac{1}{\left( {1 - \frac{2\quad b_{3}}{L}} \right)} \times \left\{ \begin{matrix} {{- {\sum\limits_{m = 1}^{N}{A_{m}^{\prime}\left( \begin{pmatrix} {{\frac{\left( {- 1} \right)^{q + m}}{\left( {q + m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\left\lbrack {2{\pi\left( {q + m} \right)}\quad\frac{1}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} -} \\ {\cos\left\lbrack {2{\pi\left( {q + m} \right)}\quad\frac{\eta}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} +} \\ {\frac{\left( {- 1} \right)^{q - m}}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\cos\left\lbrack {2\quad{\pi\left( {q - m} \right)}\frac{1}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} -} \\ {\cos\left\lbrack {2\quad{\pi\left( {q - m} \right)}\frac{\eta}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} \end{pmatrix} \right)}}} +} \\ {\underset{m \neq q}{\sum\limits_{{m = 1},}^{N}}{B_{m}^{\prime}\left( \begin{pmatrix} {{\frac{\left( {- 1} \right)^{q + m + 1}}{\left( {q + m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\sin\left\lbrack {2{\pi\left( {q + m} \right)}\quad\frac{1}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} +} \\ {\sin\left\lbrack {2{\pi\left( {q + m} \right)}\quad\frac{\eta}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} +} \\ {\frac{\left( {- 1} \right)^{q - m + 1}}{\left( {q - m} \right)\quad 2\quad\pi}\begin{Bmatrix} {{\sin\left\lbrack {2\quad{\pi\left( {q - m} \right)}\frac{1}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} +} \\ {\sin\left\lbrack {2\quad{\pi\left( {q - m} \right)}\frac{\eta}{\left( {1 + \eta} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} \end{pmatrix} \right)}} \end{matrix}\quad \right\}}}}\quad,{q \geq 1.}}\quad} & (62) \\ {{{B_{q}^{''} = {B_{q}^{\prime} + {\frac{\left( \frac{2b_{3}}{L} \right)}{\left\lbrack {1 - \left( \frac{2\quad b_{3}}{L} \right)} \right\rbrack} \times \left\{ \begin{matrix} {{\sum\limits_{m = 1}^{N}{A_{m}^{\prime}\left( \begin{pmatrix} {{\left( {- 1} \right)^{q + m + 1}\begin{Bmatrix} {\sin\quad{c\left\lbrack {{\pi\left( {q + m} \right)}\quad\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \times} \\ {\sin\left\lbrack {{\pi\left( {q + m} \right)}\quad\frac{\left( {\eta - 1} \right)}{\left( {\eta + 1} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} +} \\ {\left( {- 1} \right)^{q - m + 1}\begin{Bmatrix} {\sin\quad{c\left\lbrack {{\pi\left( {q - m} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \times} \\ {\sin\left\lbrack {{\pi\left( {q - m} \right)}\frac{\left( {\eta - 1} \right)}{\left( {\eta + 1} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} \end{pmatrix} \right)}} +} \\ {\underset{m \neq q}{\sum\limits_{{m = 1},}^{N}}{B_{m}^{\prime}\left( \begin{pmatrix} {{{- \left( {- 1} \right)^{q + m + 1}}\begin{Bmatrix} {\sin\quad{c\left\lbrack {{\pi\left( {q + m} \right)}\quad\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \times} \\ {\cos\left\lbrack {{\pi\left( {q + m} \right)}\quad\frac{\left( {\eta - 1} \right)}{\left( {\eta + 1} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} +} \\ {\left( {- 1} \right)^{q - m + 1}\begin{Bmatrix} {\sin\quad{c\left\lbrack \quad{{\pi\left( {q - m} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \times} \\ {\cos\left\lbrack {{\pi\left( {q - m} \right)}\frac{\left( {\eta - 1} \right)}{\left( {\eta + 1} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack} \end{Bmatrix}} \end{pmatrix} \right)}} \end{matrix}\quad \right\}}}}\quad,{q \geq 1.}}\quad} & (63) \end{matrix}$

The effects of non-orthogonality of functions cos(m2πy/L) and sin (m2πy/L) over the domain of y in SPD (y,{overscore (l)}_(z)=0) are evident upon examination of Equations (59) and (63). The effects of non-orthogonality are represented by the differences (A_(q)″−A_(q)′) and (B_(q)″−B_(q)′) in Equations (59) and (63), respectively.

Equations (59) and (63) can be solved for the A_(q)′ and B_(q)′, respectively, by an iterative procedure. The degree to which the effects of non-orthogonality are decoupled from the leading A_(q)′ and B_(q)′ terms in Equations (59) and (63) depends on the ratio (2b₃/L). The larger coefficients of “off diagonal terms” in Equations (59) and (63) generally occur for small values |q−m| and the relative magnitude r of the coefficients of these terms is $\begin{matrix} {r \cong {\frac{\left( \frac{2b_{3}}{L} \right)}{1 - \left( \frac{2b_{3}}{L} \right)}\sin\quad{{c\left\lbrack {{\pi\left( {q - m} \right)}\left( \frac{2b_{3}}{L} \right)} \right\rbrack}.}}} & (64) \end{matrix}$

The iterative procedure is a nontrivial step for which two solutions are given. The step is nontrivial since cos(m2πy/L) and sin (m2πy/L) are functions that are not orthogonal as a set over the domain of integration in y. One solution involves using a surface figure function ξ obtained at an earlier time based on measured values of SDP, SDP₁ ^(e), and SDP₂ ^(e) to compute values for the off-diagonal terms in Equations (59) and (63).

Alternatively, or additionally, information about a surface figure can be obtained using other techniques, such as based on values of a FDP such as given by Equation (3) or from interferometric measurements made ex-situ, e.g., a Fizeau interferometer, before the stage mirror is installed in a lithography tool.

The resulting values for A_(m)′ and B_(m)′ may be used without any iteration if the resulting values for A_(m)′ and B_(m)′ indicate that there has not been any significant change in the surface figure function ξ. If there has been a significant change, the resulting values for A_(m)′ and B_(m)′ are used as input information to compute the off-diagonal terms in a second step of the iterative procedure. The iterative steps are repeated until stable, i.e., asymptotic, values for A_(m)′ and B_(m) 40 are obtained. The values for A_(m) and B_(m) are subsequently obtained using Equations (17) and (18) from the coefficients A_(m)′ and B_(m)′ produced by the iterative procedure.

After the surface figure function ξ(y, l_(z)=0) is determined for the specified section of the x-axis stage mirror, the procedure can be repeated for other sections of the x-axis stage mirror that are used in the respective lithography tool.

In some embodiments, measured values of SDP can be used to extend a known surface figure function ξ to other sections of the x-axis stage mirror. Equation (7) allows the generation of figure error function ξ(y, l_(z)=0) for the other sections of the x-axis stage mirror from the known surface figure function ξ(y, l_(z)=0) in an adjacent section of the x-axis stage mirror.

In certain embodiments, local spatial derivatives of a surface figure function can be measured using the methods disclosed herein, in some cases, with relatively high sensitivity. The sensitivity of the third order term represented by the last term in Equation (16) is proportional to m and is equal, for example, to the sensitivity of the remaining first order terms in Equation (16) for m≈100 for |l_(z)|=0.5 milliradians and x=0.7. To measure the local spatial derivatives directly or with a higher sensitivity, the procedure described for the determination of ξ(y, l_(z)=0) can be repeated for non-zero values of l_(z) and for large values of x and y for the x-axis and y-axis stage mirrors, respectively.

The surface figure function ξ(y, {overscore (l)}_(z)=0) obtained in the above described procedures includes in particular information about ξ(y, {overscore (l)}_(z)=0) that is quadratic in y. However, the surface figure function ξ(y, {overscore (l)}_(z)=0) obtained in the above described procedure does not represent any error in ξ(y, {overscore (l)}_(z)=0) that is linear in y since SDP is zero for a plane mirror surface.

The error in the determined ξ(y, {overscore (l)}_(z)=0) linear in y relative to the error in the determined ξ(x, {overscore (l)}_(z)=0) linear in x for the x-axis and the y-axis stage mirrors, respectively, i.e., a differential error, is the only portion of the linear error that is relevant. A common mode error corresponds to a rotation of the stage. The differential error is related to the angle between the x-axis and y-axis stage mirrors and the effect of the differential error is compensated by measuring the angle between the two stage mirrors. The angle between the two stage mirrors can be measured by use of an alignment wafer and the alignment wafer rotated by 90 degrees for each plane defined by the multiple-axes/plane interferometers.

It is the information about the angles between the two stage mirrors that is used for compensating surface figure functions in yaw. Additional information about the respective surface figure functions may also be obtained by introducing a displacement of the second pass measurement beams at the stage mirror by changing the orientation of the stage mirror to change the respective pitch and repeating the procedures described herein to determine the surface figure functions at the position of the sheared measurement beams.

Values of l_(z)(y) are measured by the y-axis interferometer. During a scan of the x-axis mirror, typically there is nominally no change in the location stage in the x direction. Accordingly, there is no change in the nominal location of the measurement beams of the y-axis interferometer on the surface of the corresponding y-axis stage mirror. However, the relative scales of the measurement axes of the y-axis interferometer used to measure l_(z)(y) will not, in general, be identical and furthermore may be a function of y. The respective scales may be different due to geometric effects such as described in commonly owned U.S. patent application Ser. No. 10/872,304 entitled “COMPENSATION FOR GEOMETRIC EFFECTS OF BEAM MISALIGNMENTS IN PLANE MIRROR INTERFEROMETER METROLOGY SYSTEMS” or due to stationary systematic changes in the density gradients of the gas in the y-axis interferometer measurement beam paths.

Such errors due to relative scale errors can be difficult to measure and are typically done using an alignment wafer. However, measured values of the SDP and values of SDP reconstructed from the derived mirror surface figure functions can be used to test to see if such errors are present and if so, measure the y dependence of the relative scale errors that are quadratic and higher order in terms of y. Over time scales short compared to the time scales for changes in (E₁−E₃), the difference between measured values of SDP and values of SDP reconstructed from the derived mirror surface figure functions are obtained as a function of y. Relative scaling errors in the y axes interferometer measurements which result in l_(z)(y) having a quadratic error term with respect to y can be identified as a term linear in y for the difference between measured and reconstructed values of SDP. Similarly errors in l_(z)(y) which are cubic and higher order with respect to y can be identified as quadratic and higher order terms in y for the difference between measured and reconstructed values of SDP.

The procedure described for determining and compensating errors in the measured values of l_(z)(y) can also include compensating the effects of stationary effects of the gas in the respective measurement and reference beam paths, such as described in U.S. patent application Ser. No. 11/365,991, entitled “INTERFEROMETRY SYSTEMS AND METHODS OF USING INTERFEROMETRY SYSTEMS,” filed on Mar. 1, 2006, the entire contents of which is incorporated herein by reference.

The surface figure function for an x-axis stage mirror will, in general, be a function of both y and z and the surface figure function for the y-axis stage mirror will in general be a function of both x and z. The generalization to cover the z dependent properties is subsequently addressed by the use of a two three-axis/plane interferometer system in conjunction with a procedure to measure the angle between the x-axis and y-axis stage mirrors in two different parallel planes corresponding to the two planes defined by the two three-axis/plane interferometer system.

Once determined, surface figure functions are typically used to compensate interferometry system measurements, thereby improving an interferometry system's accuracy. For example, ξ(y) can be used to compensate measurements of the position of an x-axis stage mirror along, e.g., axis x₁ for a position y based on the following equations. If d is the true x-axis displacement of the stage mirror and ξ′(y) is the true surface figure function, an uncorrected measurement at position y, will give, for example, $\begin{matrix} {{{{\overset{\sim}{x}}_{1}(y)} = {d + \left( \frac{{\xi_{1}^{\prime}(y)} + {\xi_{0}^{\prime}(y)}}{2} \right) + {d_{nom}{\theta_{z}\left( {\frac{\partial\xi_{1}^{\prime}}{\partial y} - \frac{\partial\xi_{0}^{\prime}}{\partial y}} \right)}}}},} & (65) \end{matrix}$ where the lowest order terms dependent on the mirror surface figure function have been shown. ξ′₁ and ξ′₀ refer to the surface figure function values at positions x′₁ and x′₀, respectively, and d_(nom) is a nominal displacement value used to calculate the geometric error term that occurs for non-zero θ_(z).

Using the surface figure function, a compensated displacement x_(c)(y) can be calculated from the measured displacement based on the following equation: $\begin{matrix} {{x_{c}(y)} = {{{\overset{\sim}{x}}_{1}(y)} - \left( \frac{{\xi_{1}(y)} + {\xi_{0}(y)}}{2} \right) - {d_{nom}{{\theta_{z}\left( {\frac{\partial\xi_{1}}{\partial y} - \frac{\partial\xi_{0}}{\partial y}} \right)}.}}}} & (66) \end{matrix}$ where the lowest order terms dependent on the mirror surface figure have been shown. In embodiments, various other error compensation techniques can be used to reduce other sources of error in interferometer measurements. For example, cyclic errors that are present in the linear displacement measurements can be reduced (e.g., eliminated) and/or compensated by use of one of more techniques such as described in commonly owned U.S. patent application Ser. No. 10/097,365, entitled “CYCLIC ERROR REDUCTION IN AVERAGE INTERFEROMETRIC MEASUREMENTS,” and U.S. patent application Ser. No. 10/616,504 entitled “CYCLIC ERROR COMPENSATION IN INTERFEROMETRY SYSTEMS,” which claims priority to Provisional Patent Application No. 60/394,418 entitled “ELECTRONIC CYCLIC ERROR COMPENSATION FOR LOW SLEW RATES,” all of which are by Henry A. Hill and the contents of which are incorporated herein in their entirety by reference.

An example of another cyclic error compensation technique is described in commonly owned U.S. patent application Ser. No. 10/287,898 entitled “INTERFEROMETRIC CYCLIC ERROR COMPENSATION,” which claims priority to Provisional Patent Application No. 60/337,478 entitled “CYCLIC ERROR COMPENSATION AND RESOLUTION ENHANCEMENT,” by Henry A. Hill, the contents of which are incorporated herein in their entirety by reference.

Another example of a cyclic error compensation technique is described in U.S. patent application Ser. No. 10/174,149 entitled “INTERFEROMETRY SYSTEM AND METHOD EMPLOYING AN ANGULAR DIFFERENCE IN PROPAGATION BETWEEN ORTHOGONALLY POLARIZED INPUT BEAM COMPONENTS,” which claims priority to Provisional Patent Application 60/303,299 entitled “INTERFEROMETRY SYSTEM AND METHOD EMPLOYING AN ANGULAR DIFFERENCE IN PROPAGATION BETWEEN ORTHOGONALLY POLARIZED INPUT BEAM COMPONENTS,” both by Henry A. Hill and Peter de Groot, the contents both of which are incorporated herein in their entirety by reference.

A further example of a cyclic error compensation technique is described in commonly owned Provisional Patent Application No. 60/314,490 filed entitled “TILTED INTERFEROMETER,” by Henry A. Hill, the contents of which is herein incorporated in their entirety by reference.

Other techniques for cyclic error compensation include those described in U.S. Pat. No. 6,137,574 entitled “SYSTEMS AND METHODS FOR CHARACTERIZING AND CORRECTING CYCLIC ERRORS IN DISTANCE MEASURING AND DISPERSION INTERFEROMETRY;” U.S. Patent No. U.S. Pat. No. 6,252,668 B1, entitled “SYSTEMS AND METHODS FOR QUANTIFYING NON-LINEARITIES IN INTERFEROMETRY SYSTEMS;” and U.S. Pat. No. 6,246,481, entitled “SYSTEMS AND METHODS FOR QUANTIFYING NONLINEARITIES IN INTERFEROMETRY SYSTEMS,” wherein all three are by Henry A. Hill, the contents of the three above-cited patents and patent applications are herein incorporated in their entirety by reference.

Improved statistical accuracy in measured values of SDP can be obtained by taking advantage of the relatively low bandwidth of measured values of SDP compared to the bandwidth of the corresponding linear displacement measurements using averaging or low pass filtering. The relatively low bandwidth arises because of SDP invariance with respect to displacements of the mirror along the measurement axes and it invariance (at least to second order) on rotations of the mirror. Variations in SDP occur primarily as a result of variations of the mirror surface figure as the mirror is scanned orthogonally to the measurement axes, which depends on the mirror scan speed, but generally occurs at much lower rates than the sampling rates of the detectors used in the three-axis/plane interferometer. For example, where the 1/e² beam diameter is 5 mm and the stage is scanned at a rate of 0.5 m/s, the bandwidth of measured values of SDP will be of the order of 100 Hz compared to typical sampling rates of the respective detectors of the order of 10 MHz.

The effects of offset errors in the measured values of SDP can be measured by use of an alignment wafer and the alignment wafer rotated by 180 degrees and the offset error effects compensated. Offset errors arise in SDP because SDP is derived from three different interferometer measurements where each of the three interferometers can only measure relative changes in a respective reference and measurement beam paths. In addition, the offset errors may change with time because the calibrations of each of the three interferometers may change with respect to each other, e.g. due to changes in temperature. An alignment wafer is a wafer that includes several alignment marks that are precisely spaced with respect to each other. Accordingly, a metrology system can be calibrated by locating the marks with the system's alignment sensor and comparing the displacement between each alignment mark as measured using the metrology system with the known displacement. Because of offset errors in the interferometer distance measurements and because the angle between the measurement axes of the x-axis and y-axis interferometers is not generally known, the angle between the x-axis and y-axis stage mirrors should be independently measured. This angle can be measured in one or more planes according to whether interferometer system 10 comprises one or two three-axis/plane interferometers by use of an alignment wafer and the alignment wafer rotated by 90 degrees.

While the foregoing description is with regard to a particular interferometer assembly, namely interferometer 100, in general, other assemblies can also be used to obtain values for SDP and other parameters. For example, in some embodiments, an interferometer assembly can be configured to monitor the position of a measurement object along more than three coplanar axes (e.g., four or more axes, five or more axes). Moreover, while interferometer includes non-coplanar measurement axes, other embodiments can include exclusively coplanar axes. Furthermore, the relative position of the common measurement beam path is not limited to the position in interferometer 100. For example, in some embodiments, the common measurement beam path can be an outermost path, instead of being flanked by beam paths on either side within the common plane.

In certain embodiments, individual, rather than compound, optical components can be used. For example, free-standing beam splitters can be used to divide the first path measurement beam into the other measurement beams. Such a configuration may allow one to adjust the relative spacing of the beams, and hence the relative spacing of the measurement axes in a multi-axis interferometer.

In some embodiments, multiple single axis interferometers can be used instead of a multi-axis interferometer. For example, a three-axis/plane interferometer can be replaced by three single axis interferometers (e.g., high stability plane mirror interferometers), arranged so that each interferometer's axis lies in a common plane.

As discussed previously, lithography tools are especially useful in lithography applications used in fabricating large scale integrated circuits such as computer chips and the like. Lithography is the key technology driver for the semiconductor manufacturing industry. Overlay improvement is one of the five most difficult challenges down to and below 100 nm line widths (design rules), see, for example, the Semiconductor Industry Roadmap, p. 82 (1997).

Overlay depends directly on the performance, i.e., accuracy and precision, of the distance measuring interferometers used to position the wafer and reticle (or mask) stages. Since a lithography tool may produce $50-100M/year of product, the economic value from improved performance distance measuring interferometers is substantial. Each 1% increase in yield of the lithography tool results in approximately $1M/year economic benefit to the integrated circuit manufacturer and substantial competitive advantage to the lithography tool vendor.

The function of a lithography tool is to direct spatially patterned radiation onto a photoresist-coated wafer. The process involves determining which location of the wafer is to receive the radiation (alignment) and applying the radiation to the photoresist at that location (exposure).

To properly position the wafer, the wafer includes alignment marks on the wafer that can be measured by dedicated sensors. The measured positions of the alignment marks define the location of the wafer within the tool. This information, along with a specification of the desired patterning of the wafer surface, guides the alignment of the wafer relative to the spatially patterned radiation. Based on such information, a translatable stage supporting the photoresist-coated wafer moves the wafer such that the radiation will expose the correct location of the wafer.

During exposure, a radiation source illuminates a patterned reticle, which scatters the radiation to produce the spatially patterned radiation. The reticle is also referred to as a mask, and these terms are used interchangeably below. In the case of reduction lithography, a reduction lens collects the scattered radiation and forms a reduced image of the reticle pattern. Alternatively, in the case of proximity printing, the scattered radiation propagates a small distance (typically on the order of microns) before contacting the wafer to produce a 1:1 image of the reticle pattern. The radiation initiates photo-chemical processes in the resist that convert the radiation pattern into a latent image within the resist.

Interferometry metrology systems, such as those discussed previously, are important components of the positioning mechanisms that control the position of the wafer and reticle, and register the reticle image on the wafer. If such interferometry systems include the features described above, the accuracy of distances measured by the systems can be increased and/or maintained over longer periods without offline maintenance, resulting in higher throughput due to increased yields and less tool downtime.

In general, the lithography system, also referred to as an exposure system, typically includes an illumination system and a wafer positioning system. The illumination system includes a radiation source for providing radiation such as ultraviolet, visible, x-ray, electron, or ion radiation, and a reticle or mask for imparting the pattern to the radiation, thereby generating the spatially patterned radiation. In addition, for the case of reduction lithography, the illumination system can include a lens assembly for imaging the spatially patterned radiation onto the wafer. The imaged radiation exposes resist coated onto the wafer. The illumination system also includes a mask stage for supporting the mask and a positioning system for adjusting the position of the mask stage relative to the radiation directed through the mask. The wafer positioning system includes a wafer stage for supporting the wafer and a positioning system for adjusting the position of the wafer stage relative to the imaged radiation. Fabrication of integrated circuits can include multiple exposing steps. For a general reference on lithography, see, for example, J. R. Sheats and B. W. Smith, in Microlithography: Science and Technology (Marcel Dekker, Inc., New York, 1998), the contents of which is incorporated herein by reference.

Interferometry systems that utilize the mirror mapping procedures described above can be used to precisely measure the positions of each of the wafer stage and mask stage relative to other components of the exposure system, such as the lens assembly, radiation source, or support structure. In such cases, the interferometry system can be attached to a stationary structure and the measurement object attached to a movable element such as one of the mask and wafer stages. Alternatively, the situation can be reversed, with the interferometry system attached to a movable object and the measurement object attached to a stationary object.

More generally, such interferometry systems can be used to measure the position of any one component of the exposure system relative to any other component of the exposure system, in which the interferometry system is attached to, or supported by, one of the components and the measurement object is attached, or is supported by the other of the components.

Another example of a lithography tool 1100 using an interferometry system 1126 is shown in FIG. 5. The interferometry system is used to precisely measure the position of a wafer (not shown) within an exposure system. Here, stage 1122 is used to position and support the wafer relative to an exposure station. Scanner 1100 includes a frame 1102, which carries other support structures and various components carried on those structures. An exposure base 1104 has mounted on top of it a lens housing 1106 atop of which is mounted a reticle or mask stage 1116, which is used to support a reticle or mask. A positioning system for positioning the mask relative to the exposure station is indicated schematically by element 1117. Positioning system 1117 can include, e.g., piezoelectric transducer elements and corresponding control electronics. Although, it is not included in this described embodiment, one or more of the interferometry systems described above can also be used to precisely measure the position of the mask stage as well as other moveable elements whose position must be accurately monitored in processes for fabricating lithographic structures (see supra Sheats and Smith Microlithography: Science and Technology).

Suspended below exposure base 1104 is a support base 1113 that carries wafer stage 1122. Stage 1122 includes a plane mirror 1128 for reflecting a measurement beam 1154 directed to the stage by interferometry system 1126. A positioning system for positioning stage 1122 relative to interferometry system 1126 is indicated schematically by element 1119. Positioning system 1119 can include, e.g., piezoelectric transducer elements and corresponding control electronics. The measurement beam reflects back to the interferometry system, which is mounted on exposure base 1104. The interferometry system can be any of the embodiments described previously.

During operation, a radiation beam 1110, e.g., an ultraviolet (UV) beam from a UV laser (not shown), passes through a beam shaping optics assembly 1112 and travels downward after reflecting from mirror 1114. Thereafter, the radiation beam passes through a mask (not shown) carried by mask stage 1116. The mask (not shown) is imaged onto a wafer (not shown) on wafer stage 1122 via a lens assembly 1108 carried in a lens housing 1106. Base 1104 and the various components supported by it are isolated from environmental vibrations by a damping system depicted by spring 1120.

In other embodiments of the lithographic scanner, one or more of the interferometry systems described previously can be used to measure distance along multiple axes and angles associated for example with, but not limited to, the wafer and reticle (or mask) stages. Also, rather than a UV laser beam, other beams can be used to expose the wafer including, e.g., x-ray beams, electron beams, ion beams, and visible optical beams.

In some embodiments, the lithographic scanner can include what is known in the art as a column reference. In such embodiments, the interferometry system 1126 directs the reference beam (not shown) along an external reference path that contacts a reference mirror (not shown) mounted on some structure that directs the radiation beam, e.g., lens housing 1106. The reference mirror reflects the reference beam back to the interferometry system. The interference signal produce by interferometry system 1126 when combining measurement beam 1154 reflected from stage 1122 and the reference beam reflected from a reference mirror mounted on the lens housing 1106 indicates changes in the position of the stage relative to the radiation beam. Furthermore, in other embodiments the interferometry system 1126 can be positioned to measure changes in the position of reticle (or mask) stage 1116 or other movable components of the scanner system. Finally, the interferometry systems can be used in a similar fashion with lithography systems involving steppers, in addition to, or rather than, scanners.

As is well known in the art, lithography is a critical part of manufacturing methods for making semiconducting devices. For example, U.S. Pat. No. 5,483,343 outlines steps for such manufacturing methods. These steps are described below with reference to FIGS. 6 a and 6 b. FIG. 6 a is a flow chart of the sequence of manufacturing a semiconductor device such as a semiconductor chip (e.g., IC or LSI), a liquid crystal panel or a CCD. Step 1151 is a design process for designing the circuit of a semiconductor device. Step 1152 is a process for manufacturing a mask on the basis of the circuit pattern design. Step 1153 is a process for manufacturing a wafer by using a material such as silicon.

Step 1154 is a wafer process which is called a pre-process wherein, by using the so prepared mask and wafer, circuits are formed on the wafer through lithography. To form circuits on the wafer that correspond with sufficient spatial resolution those patterns on the mask, interferometric positioning of the lithography tool relative the wafer is necessary. The interferometry methods and systems described herein can be especially useful to improve the effectiveness of the lithography used in the wafer process.

Step 1155 is an assembling step, which is called a post-process wherein the wafer processed by step 1154 is formed into semiconductor chips. This step includes assembling (dicing and bonding) and packaging (chip sealing). Step 1156 is an inspection step wherein operability check, durability check and so on of the semiconductor devices produced by step 1155 are carried out. With these processes, semiconductor devices are finished and they are shipped (step 1157).

FIG. 6 b is a flow chart showing details of the wafer process. Step 1161 is an oxidation process for oxidizing the surface of a wafer. Step 1162 is a CVD process for forming an insulating film on the wafer surface. Step 1163 is an electrode forming process for forming electrodes on the wafer by vapor deposition. Step 1164 is an ion implanting process for implanting ions to the wafer. Step 1165 is a resist process for applying a resist (photosensitive material) to the wafer. Step 1166 is an exposure process for printing, by exposure (i.e., lithography), the circuit pattern of the mask on the wafer through the exposure apparatus described above. Once again, as described above, the use of the interferometry systems and methods described herein improve the accuracy and resolution of such lithography steps.

Step 1167 is a developing process for developing the exposed wafer. Step 1168 is an etching process for removing portions other than the developed resist image. Step 1169 is a resist separation process for separating the resist material remaining on the wafer after being subjected to the etching process. By repeating these processes, circuit patterns are formed and superimposed on the wafer.

The interferometry systems described above can also be used in other applications in which the relative position of an object needs to be measured precisely. For example, in applications in which a write beam such as a laser, x-ray, ion, or electron beam, marks a pattern onto a substrate as either the substrate or beam moves, the interferometry systems can be used to measure the relative movement between the substrate and write beam.

As an example, a schematic of a beam writing system 1200 is shown in FIG. 7. A source 1210 generates a write beam 1212, and a beam focusing assembly 1214 directs the radiation beam to a substrate 1216 supported by a movable stage 1218. To determine the relative position of the stage, an interferometry system 1220 directs a reference beam 1222 to a mirror 1224 mounted on beam focusing assembly 1214 and a measurement beam 1226 to a mirror 1228 mounted on stage 1218. Since the reference beam contacts a mirror mounted on the beam focusing assembly, the beam writing system is an example of a system that uses a column reference. Interferometry system 1220 can be any of the interferometry systems described previously. Changes in the position measured by the interferometry system correspond to changes in the relative position of write beam 1212 on substrate 1216. Interferometry system 1220 sends a measurement signal 1232 to controller 1230 that is indicative of the relative position of write beam 1212 on substrate 1216. Controller 1230 sends an output signal 1234 to a base 1236 that supports and positions stage 1218. In addition, controller 1230 sends a signal 1238 to source 1210 to vary the intensity of, or block, write beam 1212 so that the write beam contacts the substrate with an intensity sufficient to cause photophysical or photochemical change only at selected positions of the substrate.

Furthermore, in some embodiments, controller 1230 can cause beam focusing assembly 1214 to scan the write beam over a region of the substrate, e.g., using signal 1244. As a result, controller 1230 directs the other components of the system to pattern the substrate. The patterning is typically based on an electronic design pattern stored in the controller. In some applications the write beam patterns a resist coated on the substrate and in other applications the write beam directly patterns, e.g., etches, the substrate.

An important application of such a system is the fabrication of masks and reticles used in the lithography methods described previously. For example, to fabricate a lithography mask an electron beam can be used to pattern a chromium-coated glass substrate. In such cases where the write beam is an electron beam, the beam writing system encloses the electron beam path in a vacuum. Also, in cases where the write beam is, e.g., an electron or ion beam, the beam focusing assembly includes electric field generators such as quadrapole lenses for focusing and directing the charged particles onto the substrate under vacuum. In other cases where the write beam is a radiation beam, e.g., x-ray, UV, or visible radiation, the beam focusing assembly includes corresponding optics and for focusing and directing the radiation to the substrate.

A number of embodiments of the invention have been described. Nevertheless, it will be understood that various modifications may be made without departing from the spirit and scope of the invention. Accordingly, other embodiments are within the scope of the following claims. 

1. A method, comprising: locating a plurality of alignment marks on a moveable stage; interferometrically measuring a position of a measurement object along an interferometer axis for each of the alignment mark locations; and using the interferometric position measurements to derive information about a surface figure of the measurement object, wherein the position of the measurement object is measured using an interferometry assembly and either the measurement object or the interferometry assembly are attached to the stage.
 2. The method of claim 1 wherein the information comprises information related to a certain spatial frequency component of the surface figure of the measurement object.
 3. The method of claim 1 further comprising using the information to determine the surface figure of the measurement object.
 4. The method of claim 3 wherein the surface figure of the measurement object is determined based on values of a parameter associated with a displacement of the measurement object along three different measurement axes in addition to the information.
 5. The method of claim 4 wherein the parameter values are determined by interferometrically monitoring the displacement of the measurement object along each of the three different interferometer axes while moving the measurement object relative to the interferometry assembly; and determining the parameter values for different positions of the measurement object from the monitored displacements, wherein for a given position the parameter is based on the displacements of the measurement object along each of the three different interferometer axes at the given position.
 6. The method of claim 5 wherein the surface figure of the measurement object is determined based on a frequency transform of the parameter values.
 7. The method of claim 6 wherein the frequency transform is a Fourier transform.
 8. The method of claim 6 wherein the information comprises information related to a certain spatial frequency component of the surface figure of the measurement object at which the frequency transform of the parameter values is substantially insensitive.
 9. The method of claim 4 wherein the parameter is a second difference parameter.
 10. The method of claim 1 wherein the plurality of alignment marks comprises a linear array of alignment marks.
 11. The method of claim 10 wherein the linear array of the alignment marks are nominally parallel to the measurement object during the measuring.
 12. The method of claim 10 wherein adjacent alignment marks in the linear array are separated by a distance, d_(a), and the information about the surface figure of the measurement object is related to a spatial frequency component of the surface figure having a spatial wavelength Λ greater than d_(a).
 13. The method of claim 12 wherein Λ=4d_(a).
 14. The method of claim 1 wherein the alignment marks are located on the surface of an object supported by the moveable stage, and locating the alignment marks includes locating the alignment marks for at least two different positions of the object.
 15. The method of claim 14 wherein the two different object positions include a first position and a second position where the object is rotated 180° with respect to the first position.
 16. The method of claim 14 wherein the two different object positions include a first position and a second position where the object is translated relative to the first position.
 17. The method of claim 16 wherein the translation is by an amount related to a spacing of the alignment marks.
 18. The method of claim 1 further comprising using the information about the surface figure of the measurement object to improve the accuracy of measurements made using the interferometry assembly and the measurement object.
 19. The method of claim 1 further comprising using a lithography tool to expose a substrate supported by the moveable stage with a radiation pattern while interferometrically monitoring a distance between the interferometry assembly and the measurement object, wherein the position of the substrate relative to a reference frame is related to the distance between the interferometry assembly and the measurement object.
 20. A lithography method for use in fabricating integrated circuits on a wafer, the method comprising: supporting the wafer on a moveable stage; imaging spatially patterned radiation onto the wafer; adjusting the position of the stage; and monitoring the position of the stage using a measurement object and information about the surface figure of the measurement object derived using the method of claim 1 to improve the accuracy of the monitored position of the stage.
 21. A lithography method for use in the fabrication of integrated circuits comprising: directing input radiation through a mask to produce spatially patterned radiation; positioning the mask relative to the input radiation; monitoring the position of the mask relative to the input radiation using a measurement object and information about the surface figure of the measurement object derived using the method of claim 1 to improve the accuracy of the monitored position of the mask; and imaging the spatially patterned radiation onto a wafer.
 22. A lithography method for fabricating integrated circuits on a wafer comprising: positioning a first component of a lithography system relative to a second component of a lithography system to expose the wafer to spatially patterned radiation; and monitoring the position of the first component relative to the second component using a measurement object and using information about the surface figure of the measurement object derived using the method of claim 1 to improve the accuracy of the monitored position of the first component.
 23. A method for fabricating integrated circuits comprising: applying a resist to a wafer; forming a pattern of a mask in the resist by exposing the wafer to radiation using the lithography method of claim 20; and producing an integrated circuit from the wafer.
 24. A method for fabricating integrated circuits comprising: applying a resist to a wafer; forming a pattern of a mask in the resist by exposing the wafer to radiation using the lithography method of claim 21; and producing an integrated circuit from the wafer.
 25. A method for fabricating integrated circuits comprising: applying a resist to a wafer; forming a pattern of a mask in the resist by exposing the wafer to radiation using the lithography method of claim 22; and producing an integrated circuit from the wafer.
 26. A system, comprising: a moveable stage; an alignment sensor configured to locate alignment marks associated with the moveable stage; a interferometer assembly configured to produce three output beams each including interferometric information about a distance between the interferometer and a measurement object along a respective axis, the interferometer assembly or the measurement object being attached to the moveable stage; and an electronic processor configured to derive information about a surface figure of the measurement object based on data acquired by locating the plurality of alignment marks with the alignment sensor and measuring the position of the measurement object along one of the respective axes of the interferometer assembly for each of the alignment mark locations.
 27. The system of claim 26 wherein the measurement object is a plane mirror.
 28. The system of claim 26 wherein a surface of the stage includes the alignment marks.
 29. The system of claim 26 wherein the stage is configured to support an object that includes the alignment marks.
 30. The system of claim 26 wherein the alignment sensor is an optical alignment sensor.
 31. The system of claim 26 wherein the optical alignment sensor comprises a microscope.
 32. A lithography system for use in fabricating integrated circuits on a wafer, the system comprising: the system of claim 26; an illumination system for imaging spatially patterned radiation onto a wafer supported by the moveable stage; and a positioning system for adjusting the position of the stage relative to the imaged radiation; wherein the interferometer assembly is configured to monitor the position of the wafer relative to the imaged radiation and electronic processor is configured to use the information about the surface figure of the measurement object to improve the accuracy of the monitored position of the wafer.
 33. A method for fabricating integrated circuits comprising: applying a resist to a wafer; forming a pattern of a mask in the resist by exposing the wafer to radiation using the lithography system of claim 32; and producing an integrated circuit from the wafer.
 34. A beam writing system for use in fabricating a lithography mask, the system comprising: the system of claim 26; a source providing a write beam to pattern a substrate supported by the moveable stage; a beam directing assembly for delivering the write beam to the substrate; a positioning system for positioning the stage and beam directing assembly relative one another; wherein the interferometer assembly is configured to monitor the position of the stage relative to the beam directing assembly and electronic processor is configured to use the information about the surface figure of the measurement object to improve the accuracy of the monitored position of the stage.
 35. A method for fabricating a lithography mask comprising: directing a beam to a substrate using the beam writing system of claim 34; varying the intensity or the position of the beam at the substrate to form a pattern in the substrate; and forming the lithography mask from the patterned substrate. 